High accuracy; supports IEC 60687/61036/61268 and
IEC 62053-21/62053-22/62053-23
On-chip digital integrator enables direct interface to current
sensors with di/dt output
Active, reactive, and apparent energy; sampled waveform;
current and voltage rms
Less than 0.1% error in active energy measurement over a
dynamic range of 1000 to 1 at 25°C
Positive-only energy accumulation mode available
On-chip user programmable threshold for line voltage surge
and SAG and PSU supervisory
Digital calibration for power, phase, and input offset
On-chip temperature sensor (±3°C typical)
SPI® compatible serial interface
Pulse output with programmable frequency
Interrupt request pin (
Reference 2.4 V with external overdrive capability
Single 5 V supply, low power (25 mW typical)
GENERAL DESCRIPTION
The ADE7753 features proprietary ADCs and DSP for high
accuracy over large variations in environmental conditions and
time. The ADE7753 incorporates two second-order 16-bit Σ-∆
ADCs, a digital integrator (on CH1), reference circuitry,
temperature sensor, and all the signal processing required to
perform active, reactive, and apparent energy measurements,
line-voltage period measurement, and rms calculation on the
IRQ
) and status register
with di/dt Sensor Interface
ADE7753
voltage and current. The selectable on-chip digital integrator
provides direct interface to di/dt current sensors such as
Rogowski coils, eliminating the need for an external analog
integrator and resulting in excellent long-term stability and precise phase matching between the current and voltage channels.
The ADE7753 provides a serial interface to read data, and a
pulse output frequency (CF), which is proportional to the active
power. Various system calibration features, i.e., channel offset
correction, phase calibration, and power calibration, ensure high
accuracy. The part also detects short duration low or high
voltage variations.
The positive-only accumulation mode gives the option to
accumulate energy only when positive power is detected. An
internal no-load threshold ensures that the part does not exhibit
any creep when there is no load. The zero-crossing output (ZX)
produces a pulse that is synchronized to the zero-crossing point
of the line voltage. This signal is used internally in the line cycle
active and apparent energy accumulation modes, which enables
faster calibration.
The interrupt status register indicates the nature of the interrupt,
and the interrupt enable register controls which event produces
IRQ
an output on the
The ADE7753 is available in a 20-lead SSOP package.
Information furnished by Analog Devices is believed to be accurate and reliable.
However, no responsibility is assumed by Analog Devices for its use, nor for any
infringements of patents or other rights of third parties that may result from its use.
Specifications subject to change without notice. No license is granted by implication
or otherwise under any patent or patent rights of Analog Devices. Trademarks and
registered trademarks are the property of their respective owners.
Active Power Measurement Error CLKIN = 3.579545 MHz
Channel 1 Range = 0.5 V Full Scale Channel 2 = 300 mV rms/60 Hz, gain = 2
Gain = 1 0.1 % typ Over a dynamic range 1000 to 1
Gain = 2 0.1 % typ Over a dynamic range 1000 to 1
Gain = 4 0.1 % typ Over a dynamic range 1000 to 1
Gain = 8 0.1 % typ Over a dynamic range 1000 to 1
Channel 1 Range = 0.25 V Full Scale
Gain = 1 0.1 % typ Over a dynamic range 1000 to 1
Gain = 2 0.1 % typ Over a dynamic range 1000 to 1
Gain = 4 0.1 % typ Over a dynamic range 1000 to 1
Gain = 8 0.2 % typ Over a dynamic range 1000 to 1
Channel 1 Range = 0.125 V Full Scale
Gain = 1 0.1 % typ Over a dynamic range 1000 to 1
Gain = 2 0.1 % typ Over a dynamic range 1000 to 1
Gain = 4 0.2 % typ Over a dynamic range 1000 to 1
Gain = 8 0.2 % typ Over a dynamic range 1000 to 1
Active Power Measurement Bandwidth 14 kHz
Phase Error 1 between Channels
AC Power Supply Rejection
2
2
±0.05 max Line Frequency = 45 Hz to 65 Hz, HPF on
AVDD = DVDD = 5 V + 175 mV rms/120 Hz
Output Frequency Variation (CF) 0.2 % typ Channel 1 = 20 mV rms, gain = 16, range = 0.5 V
Channel 2 = 300 mV rms/60 Hz, gain = 1
DC Power Supply Rejection
2
AVDD = DVDD = 5 V ± 250 mV dc
Output Frequency Variation (CF) ±0.3 % typ Channel 1 = 20 mV rms/60 Hz, gain = 16, range = 0.5 V
Channel 2 = 300 mV rms/60 Hz, gain = 1
IRMS Measurement Error 0.5 % typ Over a dynamic range 100 to 1
IRMS Measurement Bandwidth 14 kHz
VRMS Measurement Error 0.5 % typ Over a dynamic range 20 to 1
VRMS Measurement Bandwidth 140 Hz
ANALOG INPUTS
3
See the Analog Inputs section
Maximum Signal Levels ±0.5 V max V1P, V1N, V2N, and V2P to AGND
Input Impedance (dc) 390 k min
Bandwidth 14 kHz CLKIN/256, CLKIN = 3.579545 MHz
Gain Error
2, 3
External 2.5 V reference, gain = 1 on Channels 1 and 2
Channel 1
Range = 0.5 V Full Scale ±4 % typ V1 = 0.5 V dc
Range = 0.25 V Full Scale ±4 % typ V1 = 0.25 V dc
Range = 0.125 V Full Scale ±4 % typ V1 = 0.125 V dc
Channel 2 ±4 % typ V2 = 0.5 V dc
Offset Error
2
±32 mV max Gain 1
Channel 1 ±13 mV max Gain 16
±32 mV max Gain 1
Channel 2 ±13 mV max Gain 16
Reference Error ±200 mV max
Current Source 10 µA max
Output Impedance 3.4 kΩ min
Temperature Coefficient 30 ppm/°C typ
CLKIN All specifications CLKIN of 3.579545 MHz
Input Clock Frequency 4 MHz max
1 MHz min
LOGIC INPUTS
RESET
Input High Voltage, V
Input Low Voltage, V
Input Current, I
Input Capacitance, C
LOGIC OUTPUTS
SAG
Output High Voltage, V
Output Low Voltage, V
ZX and DOUT
Output High Voltage, V
Output Low Voltage, V
CF
Output High Voltage, V
Output Low Voltage, V
POWER SUPPLY For specified performance
AVDD 4.75 V min 5 V – 5%
5.25 V max 5 V + 5%
DVDD 4.75 V min 5 V – 5%
5.25 V max 5 V + 5%
AI
DI
_______________________________________________
1
See the plots in the Typical Performance Characteristics section.
2
See the Terminology section for explanation of specifications.
3
See the Analog Inputs section.
Input Voltage Range 2.6 V max 2.4 V + 8%
IN/OUT
, DIN, SCLK, CLKIN, and
IN
IRQ
and
DD
DD
CS
INH
INL
IN
OH
OL
OH
OL
OH
OL
2.4 V min DVDD = 5 V ± 10%
0.8 V max DVDD = 5 V ± 10%
±3 µA max Typically 10 nA, VIN = 0 V to DV
10 pF max
Open-drain outputs, 10 kΩ pull-up resistor
4 V min I
0.4 V max I
4 V min I
0.4 V max I
4 V min I
1 V max I
3 mA max Typically 2.0 mA
4 mA max Typically 3.0 mA
200 µA
SOURCE
= 0.8 mA
SINK
SOURCE
= 0.8 mA
SINK
SOURCE
= 7 mA
SINK
I
Ol
= 5 mA
= 5 mA
= 5 mA
IN/OUT
pin
DD
OUTPUT
PIN
TO
50pF
C
L
1.6mA
I
OH
+2.1V
02875-0-002
Figure 2. Load Circuit for Timing Specifications
Rev. A | Page 4 of 60
Page 5
ADE7753
K
TIMING CHARACTERISTICS
AVDD = DV = 5 V ± 5%, AGND = DGND = 0 V, on-chip reference, CLKIN = 3.579545 MHz XTAL, T
DDMIN
Table 2.
Parameter
1, 2
Spec Unit Test Conditions/Comments
Write Timing
t
1
t
2
t
3
t
4
t
5
t
6
t
7
t
8
50 ns (min)
CS falling edge to first SCLK falling edge.
50 ns (min) SCLK logic high pulse width.
50 ns (min) SCLK logic low pulse width.
10 ns (min) Valid data setup time before falling edge of SCLK.
5 ns (min) Data hold time after SCLK falling edge.
400 ns (min) Minimum time between the end of data byte transfers.
50 ns (min) Minimum time between byte transfers during a serial write.
100 ns (min)
CS hold time after SCLK falling edge.
Read Timing
3
t
9
4 µs (min) Minimum time between read command (i.e., a write to
communication register) and data read.
t
10
t
11
50 ns (min) Minimum time between data byte transfers during a multibyte read.
30 ns (min) Data access time after SCLK rising edge following a write to the
communications register.
4
t
12
100 ns (max) Bus relinquish time after falling edge of SCLK.
10 ns (min)
5
t
13
100 ns (max)
Bus relinquish time after rising edge of
10 ns (min)
___________________________________
1
Sample tested during initial release and after any redesign or process change that could affect this parameter. All input signals are specified with tr = tf = 5 ns
(10% to 90%) and timed from a voltage level of 1.6 V.
2
See Figure 3, Figure 4, and the ADE7753 Serial Interface section.
3
Minimum time between read command and data read for all registers except waveform register, which is t9 = 500 ns min.
4
Measured with the load circuit in Figure 2 and defined as the time required for the output to cross 0.8 V or 2.4 V.
5
Derived from the measured time taken by the data outputs to change 0.5 V when loaded with the circuit in Figure 2. The measured number is then extrapolated back
to remove the effects of charging or discharging the 50 pF capacitor. This means that the time quoted in the timing characteristics is the true bus relinquish time of
the part and is independent of the bus loading.
CS
SCL
DIN
t
1
1
t
3
t
A4A5A3
4
t
5
A2
A1
t
2
0
t
7
A0
DB7
DB0
t
7
DB7
to T
t
6
= –40°C to +85°C.
MAX
CS
.
t
8
DB0
COMMAND BYTE
MOST SIGNIFICANT BYTE
LEAST SIGNIFICANT BYTE
02875-0-081
Figure 3. Serial Write Timing
CS
SCLK
DIN
DOUT
t
1
t
9
0
0
A4A5A3
COMMAND BYTE
A2
A0
A1
t
11
DB7
MOST SIGNIFICANT BYTE
t
10
t
11
DB0
LEAST SIGNIFICANT BYTE
t
13
t
12
DB0DB7
02875-0-083
Figure 4. Serial Read Timing
Rev. A | Page 5 of 60
Page 6
ADE7753
ABSOLUTE MAXIMUM RATINGS
T = 25°C, unless otherwise noted.
A
Table 3.
Parameter Rating
AVDD to AGND –0.3 V to +7 V
DVDD to DGND –0.3 V to +7 V
DVDD to AVDD –0.3 V to +0.3 V
Analog Input Voltage to AGND
V1P, V1N, V2P, and V2N
Reference Input Voltage to AGND –0.3 V to AVDD + 0.3 V
Digital Input Voltage to DGND –0.3 V to DVDD + 0.3 V
Digital Output Voltage to DGND –0.3 V to DVDD + 0.3 V
Operating Temperature Range Industrial –40°C to +85°C
Storage Temperature Range –65°C to +150°C
Junction Temperature 150°C
20-Lead SSOP, Power Dissipation 450 mW
θJA Thermal Impedance 112°C/W
Lead Temperature, Soldering Vapor Phase (60 sec) 215°C
Infrared (15 sec) 220°C
–6 V to +6 V
Stresses above those listed under Absolute Maximum Ratings
may cause permanent damage to the device. This is a stress
rating only and functional operation of the device at these or
any other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect
device reliability.
ESD CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily accumulate on
the human body and test equipment and can discharge without detection. Although this product features
proprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energy
electrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance
degradation or loss of functionality.
Rev. A | Page 6 of 60
Page 7
ADE7753
TERMINOLOGY
Measurement Error
The error associated with the energy measurement made by the
ADE7753 is defined by the following formula:
⎛
⎜
ErrorPercentage
=
⎜
⎝
EnergyTrue
7753
−
⎞
EnergyTrueADERegisterEnergy
⎟
%100
×
⎟
⎠
supplies. Any error introduced by this ac signal is expressed as
a percentage of reading—see the Measurement Error definition.
For the dc PSR measurement, a reading at nominal supplies
(5 V) is taken. A second reading is obtained with the same input
signal levels when the supplies are varied ±5%. Any error
introduced is again expressed as a percentage of the reading.
Phase Error between Channels
The digital integrator and the high-pass filter (HPF) in Channel 1
have a non-ideal phase response. To offset this phase response
and equalize the phase response between channels, two phasecorrection networks are placed in Channel 1: one for the digital
integrator and the other for the HPF. The phase correction
networks correct the phase response of the corresponding
component and ensure a phase match between Channel 1
(current) and Channel 2 (voltage) to within ±0.1° over a range
of 45 Hz to 65 Hz with the digital integrator off. With the
digital integrator on, the phase is corrected to within ±0.4°
over a range of 45 Hz to 65 Hz.
Power Supply Rejection
This quantifies the ADE7753 measurement error as a percentage
of reading when the power supplies are varied. For the ac PSR
measurement, a reading at nominal supplies (5 V) is taken. A
second reading is obtained with the same input signal levels
when an ac (175 mV rms/120 Hz) signal is introduced onto the
ADC Offset Error
The dc offset associated with the analog inputs to the ADCs. It
means that with the analog inputs connected to AGND, the
ADCs still see a dc analog input signal. The magnitude of the
offset depends on the gain and input range selection—see the
Typical Performance Characteristics section. However, when
HPF1 is switched on, the offset is removed from Channel 1
(current) and the power calculation is not affected by this
offset. The offsets can be removed by performing an offset
calibration—see the Analog Inputs section.
Gain Error
The difference between the measured ADC output code (minus
the offset) and the ideal output code—see the Channel 1 ADC
and Channel 2 ADC sections. It is measured for each of the
input ranges on Channel 1 (0.5 V, 0.25 V, and 0.125 V). The
difference is expressed as a percentage of the ideal code.
Rev. A | Page 7 of 60
Page 8
ADE7753
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
RESET
Table 4. Pin Function Descriptions
Pin No. Mnemonic Description
1
RESET
Reset Pin for the ADE7753. A logic low on this pin holds the ADCs and digital circuitry (including the serial
interface) in a reset condition.
2 DVDD
Digital Power Supply. This pin provides the supply voltage for the digital circuitry in the ADE7753. The
supply voltage should be maintained at 5 V ± 5% for specified operation. This pin should be decoupled to
DGND with a 10 µF capacitor in parallel with a ceramic 100 nF capacitor.
3 AVDD
Analog Power Supply. This pin provides the supply voltage for the analog circuitry in the ADE7753. The
supply should be maintained at 5 V ± 5% for specified operation. Every effort should be made to minimize
power supply ripple and noise at this pin by the use of proper decoupling. The typical performance graphs
show the power supply rejection performance. This pin should be decoupled to AGND with a 10 µF
capacitor in parallel with a ceramic 100 nF capacitor.
4, 5 V1P, V1N
Analog Inputs for Channel 1. This channel is intended for use with a di/dt current transducer such as a
Rogowski coil or another current sensor such as a shunt or current transformer (CT). These inputs are fully
differential voltage inputs with maximum differential input signal levels of ±0.5 V, ±0.25 V, and ±0.125 V,
depending on the full-scale selection—see the Analog Inputs section. Channel 1 also has a PGA with gain
selections of 1, 2, 4, 8, or 16. The maximum signal level at these pins with respect to AGND is ±0.5 V. Both
inputs have internal ESD protection circuitry, and, in addition, an overvoltage of ±6 V can be sustained on
these inputs without risk of permanent damage.
6, 7 V2N, V2P
Analog Inputs for Channel 2. This channel is intended for use with the voltage transducer. These inputs are
fully differential voltage inputs with a maximum differential signal level of ±0.5 V. Channel 2 also has a PGA
with gain selections of 1, 2, 4, 8, or 16. The maximum signal level at these pins with respect to AGND is
±0.5 V. Both inputs have internal ESD protection circuitry, and an overvoltage of ±6 V can be sustained on
these inputs without risk of permanent damage.
8 AGND
Analog Ground Reference. This pin provides the ground reference for the analog circuitry in the ADE7753,
i.e., ADCs and reference. This pin should be tied to the analog ground plane or the quietest ground
reference in the system. This quiet ground reference should be used for all analog circuitry, for example,
anti-aliasing filters, current and voltage transducers, etc. To keep ground noise around the ADE7753 to a
minimum, the quiet ground plane should connected to the digital ground plane at only one point. It is
acceptable to place the entire device on the analog ground plane.
9 REF
IN/OUT
Access to the On-Chip Voltage Reference. The on-chip reference has a nominal value of 2.4 V ± 8% and a
typical temperature coefficient of 30 ppm/°C. An external reference source can also be connected at this
pin. In either case, this pin should be decoupled to AGND with a 1 µF ceramic capacitor.
10 DGND
Digital Ground Reference. This pin provides the ground reference for the digital circuitry in the ADE7753,
i.e., multiplier, filters, and digital-to-frequency converter. Because the digital return currents in the
ADE7753 are small, it is acceptable to connect this pin to the analog ground plane of the system. However,
high bus capacitance on the DOUT pin could result in noisy digital current, which could affect
performance.
11 CF
Calibration Frequency Logic Output. The CF logic output gives active power information. This output is
intended to be used for operational and calibration purposes. The full-scale output frequency can be
adjusted by writing to the CFDEN and CFNUM registers—see the Energy-to-Frequency Conversion section.
1
2
DVDD
AVDD
3
4
V1P
ADE7753
V1N
5
TOP VIEW
6
(Not to Scale)
7
8
9
10
02875-0-005
REF
V2N
V2P
AGND
IN/OUT
DGND
Figure 5. Pin Configuration (SSOP Package)
DIN
20
19
DOUT
SCLK
18
17
CS
CLKOUT
16
CLKIN
15
14
IRQ
SAG
13
ZX
12
CF
11
Rev. A | Page 8 of 60
Page 9
ADE7753
Pin No. Mnemonic Description
12 ZX
13
14
SAGThis open-drain logic output goes active low when either no zero crossings are detected or a low voltage
IRQInterrupt Request Output. This is an active low open-drain logic output. Maskable interrupts include active
15 CLKIN
16 CLKOUT
17
CSChip Select. Part of the 4-wire SPI serial interface. This active low logic input allows the ADE7753 to share
18 SCLK
19 DOUT
20 DIN
Voltage Waveform (Channel 2) Zero-Crossing Output. This output toggles logic high and logic low at the
zero crossing of the differential signal on Channel 2—see the Zero-Crossing Detection section.
threshold (Channel 2) is crossed for a specified duration—see the Line Voltage Sag Detection section.
energy register rollover, active energy register at half level, and arrivals of new waveform samples—see the
ADE7753 Interrupts section.
Master Clock for ADCs and Digital Signal Processing. An external clock can be provided at this logic input.
Alternatively, a parallel resonant AT crystal can be connected across CLKIN and CLKOUT to provide a clock
source for the ADE7753. The clock frequency for specified operation is 3.579545 MHz. Ceramic load
capacitors of between 22 pF and 33 pF should be used with the gate oscillator circuit. Refer to the crystal
manufacturer’s data sheet for load capacitance requirements.
A crystal can be connected across this pin and CLKIN as described for Pin 15 to provide a clock source for
the ADE7753. The CLKOUT pin can drive one CMOS load when either an external clock is supplied at CLKIN
or a crystal is being used.
the serial bus with several other devices—see the ADE7753 Serial Interface section.
Serial Clock Input for the Synchronous Serial Interface. All serial data transfers are synchronized to this
clock—see the ADE7753 Serial Interface section. The SCLK has a Schmitt-trigger input for use with a clock
source that has a slow edge transition time, for example, opto-isolator output.
Data Output for the Serial Interface. Data is shifted out at this pin on the rising edge of SCLK. This logic
output is normally in a high impedance state unless it is driving data onto the serial data bus—see the
ADE7753 Serial Interface section.
Data Input for the Serial Interface. Data is shifted in at this pin on the falling edge of SCLK—see the
ADE7753 Serial Interface section.
Rev. A | Page 9 of 60
Page 10
ADE7753
TYPICAL PERFORMANCE CHARACTERISTICS
0.5
0.4
0.3
0.2
+25°C, PF = 1
0.1
0
–0.1
ERROR (%)
–0.2
–0.3
–0.4
–0.5
0.1
+85°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
Figure 6. Active Energy Error as a Percentage of Reading (Gain = 1) over
Power Factor with Internal Reference and Integrator Off
GAIN = 1
INTEGRATOR OFF
INTERNAL REFERENCE
–40°C, PF = 0.5
+25°C, PF = 0.5
02875-0-006
0.3
GAIN = 8
0.2
0.1
0
ERROR (%)
–0.1
–0.2
–0.3
0.1
+85°C, PF = 1
+25°C, PF = 1
–40°C, PF = 1
110100
FULL-SCALE CURRENT (%)
INTEGRATOR OFF
EXTERNAL REFERENCE
02875-0-010
Figure 9. Active Energy Error as a Percentage of Reading (Gain = 8) over
Temperature with External Reference and Integrator Off
0.4
0.3
0.2
0.1
0
ERROR (%)
–0.1
–0.2
–0.3
–0.4
0.1
+85°C, PF = 1
+25°C, PF = 1
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR OFF
INTERNAL REFERENCE
–40°C, PF = 1
02875-0-008
Figure 7. Active Energy as a Percentage of Reading (Gain = 8) over
Temperature with Internal Reference and Integrator Off
0.8
0.6
0.4
0.2
0
ERROR (%)
–0.2
–0.4
–0.6
0.1
+25°C, PF = 1
–40°C, PF = 0.5
+85°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR OFF
INTERNAL REFERENCE
+25°C, PF = 0.5
02875-0-009
Figure 8. Active Energy Error as a Percentage of Reading (Gain = 8) over
Power Factor with Internal Reference and Integrator Off
0.6
GAIN = 8
0.4
0.2
0
ERROR (%)
–0.2
–0.4
–0.6
0.1
+25°C, PF = 1
+25°C, PF = 0.5
+85°C, PF = 0.5
–40°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
INTEGRATOR OFF
EXTERNAL REFERENCE
02875-0-011
Figure 10. Active Energy Error as a Percentage of Reading (Gain = 8) over
Power Factor with External Reference and Integrator Off
0.5
0.4
0.3
0.2
0.1
–0.1
ERROR (%)
–0.2
–0.3
–0.4
–0.5
0
0.1
+25°C, PF = 0
–40°C, PF = 0.5
+85°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 1
INTEGRATOR OFF
INTERNAL REFERENCE
+25°C, PF = 0.5
02875-0-012
Figure 11. Reactive Energy Error as a Percentage of Reading (Gain = 1) over
Power Factor with Internal Reference and Integrator Off
Rev. A | Page 10 of 60
Page 11
ADE7753
0.5
0.4
0.3
0.2
0.1
0
–0.1
ERROR (%)
–0.2
–0.3
–0.4
–0.5
0.1
+25°C, PF = 0
+25°C, PF = 0.5
–40°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 1
INTEGRATOR OFF
EXTERNAL REFERENCE
+85°C, PF = 0.5
02875-0-013
Figure 12. Reactive Energy Error as a Percentage of Reading (Gain = 1) over
Power Factor with External Reference and Integrator Off
0.35
0.25
0.15
0.05
–0.05
ERROR (%)
–0.15
–0.25
–0.35
0.1
+85°C, PF = 0
+25°C, PF = 0
–40°C, PF = 0
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR OFF
EXTERNAL REFERENCE
02875-0-016
Figure 15. Reactive Energy Error as a Percentage of Reading (Gain = 8) over
Temperature with External Reference and Integrator Off
0.20
0.15
–40°C, PF = 0
0.10
0.05
0
ERROR (%)
–0.05
–0.10
–0.15
–0.20
0.1
+25°C, PF = 0
+85°C, PF = 0
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR OFF
INTERNAL REFERENCE
02875-0-014
Figure 13. Reactive Energy Error as a Percentage of Reading (Gain = 8) over
Temperature with Internal Reference and Integrator Off
0.3
GAIN = 8
0.2
0.1
0
ERROR (%)
–0.1
–0.2
–40°C, PF = 0.5
+25°C, PF = 0
+85°C, PF = 0.5
INTEGRATOR OFF
INTERNAL REFERENCE
+25°C, PF = 0.5
0.5
0.4
0.3
0.2
0.1
0
–0.1
ERROR (%)
–0.2
–0.3
–0.4
–0.5
0.1
+25°C, PF = 0
+85°C, PF = 0.5
–40°C, PF = 0.5
+25°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR OFF
EXTERNAL REFERENCE
02875-0-017
Figure 16. Reactive Energy Error as a Percentage of Reading (Gain = 8) over
Power Factor with External Reference and Integrator Off
0.3
0.2
0.1
0
ERROR (%)
–0.1
–0.2
5.25V
5.0V
GAIN = 8
INTEGRATOR OFF
INTERNAL REFERENCE
4.75V
–0.3
0.1
110100
FULL-SCALE CURRENT (%)
02875-0-015
Figure 14. Reactive Energy Error as a Percentage of Reading (Gain = 8) over
Power Factor with Internal Reference and Integrator Off
Rev. A | Page 11 of 60
–0.3
0.1
110100
FULL-SCALE CURRENT (%)
02875-0-018
Figure 17. Active Energy Error as a Percentage of Reading (Gain = 8) over
Power Supply with Internal Reference and Integrator O ff
Page 12
ADE7753
5
d
0.1
0.8
0.6
0.4
0.2
0
–0.2
ERROR (%)
–0.4
–0.6
–0.8
–0.1
45
5055606
PF = 1
PF = 0.5
LINE FREQUENCY (Hz)
Figure 18. Active Energy Error as a Percentage of Reading (Gain = 8) over
Frequency with External Reference and Integrator O ff
GAIN = 8
INTEGRATOR OFF
EXTERNAL REFERENCE
02875-0-019
1.0
0.8
0.6
0.4
0.2
0
–0.2
ERROR (%)
–0.4
–0.6
–0.8
–1.0
0.1
–40°C, PF = 1
85°C, PF = 1
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR ON
INTERNAL REFERENCE
25°C, PF = 1
02875-0-023
Figure 21. Active Energy Error as a Percentage of Reading (Gain = 8) over
Temperature with Internal Reference and Integrator On
0.5
0.4
0.3
0.2
0.1
0
–0.1
ERROR (%)
–0.2
–0.3
–0.4
–0.5
0.1
PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR OFF
INTERNAL REFERENCE
PF = 1
02875-0-020
Figure 19. IRMS Error as a Percentage of Reading (Gain = 8) with
Internal Reference and Integrator Off
1.0
0.8
0.6
0.4
0.2
0
–0.2
ERROR (%)
–0.4
–0.6
–0.8
–1.0
0.1
–40°C, PF = 0.5
+25°C, PF = 0.5
+85°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR ON
INTERNAL REFERENCE
+25°C, PF = 1
02875-0-022
Figure 20. Active Energy Error as a Percentage of Reading (Gain = 8) over
Power Factor with Internal Reference an
Integrator On
1.0
0.8
0.6
0.4
0.2
0
–0.2
ERROR (%)
–0.4
–0.6
–0.8
–1.0
0.1
+25°C, PF = 0
–40°C, PF = 0.5
+85°C, PF = 0.5
+25°C, PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR ON
INTERNAL REFERENCE
02875-0-024
Figure 22. Reactive Energy Error as a Percentage of Reading (Gain = 8) over
Power Factor with Internal Reference and Integrator On
1.0
0.8
0.6
0.4
0.2
0
–0.2
ERROR (%)
–0.4
–0.6
–0.8
–1.0
0.1
–40°C, PF = 0
+25°C, PF = 0
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR ON
INTERNAL REFERENCE
+85°C, PF = 0
02875-0-025
Figure 23. Reactive Energy Error as a Percentage of Reading (Gain = 8) over
Temperature with Internal Reference and Integrator On
Rev. A | Page 12 of 60
Page 13
ADE7753
3.0
2.5
2.0
1.5
1.0
0.5
0
ERROR (%)
–0.5
–1.0
–1.5
–2.0
4547495153555759616365
PF = 0.5
PF = 1
FREQUENCY (Hz)
GAIN = 8
INTEGRATOR ON
INTERNAL REFERENCE
02875-0-026
Figure 24. Active Energy Error as a Percentage of Reading (Gain = 8) over
Power Factor with Internal Reference and Integrator On
0.3
0.8
0.6
0.4
0.2
0
ERROR (%)
–0.2
–0.4
–0.6
–0.8
1
FULL-SCALE VOLTAGE
GAIN = 1
EXTERNAL REFERENCE
10100
02875-0-029
Figure 27. VRMS Error as a Percentage of Reading (Gain = 1) with
External Reference
0.2
0.1
0
ERROR (%)
–0.1
–0.2
–0.3
0.1
5.25V
5.0V
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR ON
INTERNAL REFERENCE
4.75V
02875-0-027
Figure 25. Active Energy Error as a Percentage of Reading (Gain = 8) over
Power Supply with Internal Reference and Integrator On
0.5
0.4
0.3
0.2
0.1
0
–0.1
ERROR (%)
–0.2
–0.3
–0.4
–0.5
0.1
PF = 1
PF = 0.5
110100
FULL-SCALE CURRENT (%)
GAIN = 8
INTEGRATOR ON
INTERNAL REFERENCE
02875-0-028
Figure 26. IRMS Error as a Percentage of Reading (Gain = 8) with
Internal Reference and Integrator On
8
6
HITS
4
2
0
–15–12–9–6–3
CH1 OFFSET (0p5V_1X) (mV)
036
02875-0-087
Figure 28. Channel 1 Offset (Gain = 1)
Rev. A | Page 13 of 60
Page 14
ADE7753
V
DD
I
di/dt CURRENT
SENSOR
110V
CHANNEL 1 GAIN = 8
CHANNEL 2 GAIN = 1
10µF
100Ω 1kΩ
33nF 33nF
100Ω 1kΩ
33nF
1kΩ
600kΩ
1kΩ
10µF
100nF100nF
AVDD DVDD
V1P
33nF
33nF
33nF
100nF
V1N
ADE7753
V2N
V2P
REF
IN/OUT
AGND DGND
U1
RESET
DIN
DOUT
SCLK
CS
CLKOUT
CLKIN
IRQ
SAG
ZX
CF
TOSPI BUS
(USED ONLY FOR
CALIBRATION)
Y1
3.58MHz
NOT CONNECTED
Figure 29. Test Circuit for Performance Curves with Integrator On
10µF
22pF
U3
PS2501-1
22pF
TO
FREQUENCY
COUNTER
02875-A-012
V
DD
I
110V
CT TURN RATIO = 1800:1
CHANNEL 2 GAIN = 1
GAIN 1 (CH1)
10µF1µF
CURRENT
TRANSFORMER
RB
1kΩ
600kΩ
1kΩ
10µF
1
8
100nF100nF
1kΩ
33nF
1kΩ
33nF
33nF
33nF
100nF
RB
10Ω
1.21Ω
AVDD DVDD
V1P
V1N
V2N
V2P
REF
U1
ADE7753
CLKOUT
IN/OUT
AGND DGND
RESET
DIN
DOUT
SCLK
CS
CLKIN
IRQ
SAG
ZX
CF
0
TOSPI BUS
(USED ONLY FOR
CALIBRATION)
22pF
U3
PS2501-1
22pF
TO
FREQUENCY
COUNTER
02875-0-030
Y1
3.58MHz
NOT CONNECTED
Figure 30. Test Circuit for Performance Curves with Integrator Off
Rev. A | Page 14 of 60
Page 15
ADE7753
T
THEORY OF OPERATION
ANALOG INPUTS
The ADE7753 has two fully differential voltage input channels.
The maximum differential input voltage for input pairs V1P/V1N
and V2P/V2N is ±0.5 V. In addition, the maximum signal level
on analog inputs for V1P/V1N and V2P/ V2N is ±0.5 V with
respect to AGND.
Each analog input channel has a programmable gain amplifier
(PGA) with possible gain selections of 1, 2, 4, 8, and 16. The gain
selections are made by writing to the gain register—see Figure 32.
Bits 0 to 2 select the gain for the PGA in Channel 1, and the gain
selection for the PGA in Channel 2 is made via Bits 5 to 7.
Figure 31 shows how a gain selection for Channel 1 is made
using the gain register.
76 5 4 3 2 1 0
00 0 0 0 0 0 0
V1P
V
IN
V1N
7654 3210
0000 0000
CH1OS[7:0]
BITS 0 to 5: SIGN MAGNITUDE CODED OFFSET CORRECTION
BIT 6: NOT USED
BIT 7: DIGITAL INTEGRATOR (ON = 1, OFF = 0; DEFAULT OFF)
In addition to the PGA, Channel 1 also has a full-scale input
range selection for the ADC. The ADC analog input range
selection is also made using the gain register—see Figure 32. As
mentioned previously, the maximum differential input voltage is
0.5 V. However, by using Bits 3 and 4 in the gain register, the
maximum ADC input voltage can be set to 0.5 V, 0.25 V, or
0.125 V. This is achieved by adjusting the ADC reference—see
the ADE7753 Reference Circuit section. Table 5 summarizes the
maximum differential input signal level on Channel 1 for the
various ADC range and gain selections.
GAIN[7:0]
GAIN (K)
SELECTION
K × V
IN
Figure 31. PGA in Channel 1
+
OFFSET ADJUST
(±50mV)
02875-0-031
Table 5. Maximum Input Signal Levels for Channel 1
Max Signal ADC Input Range Selection
Channel 1 0.5 V 0.25 V 0.125 V
It is also possible to adjust offset errors on Channel 1 and
Channel 2 by writing to the offset correction registers, CH1OS
and CH2OS, respectively. These registers allow channel offsets
in the range ±20 mV to ±50 mV (depending on the gain setting)
to be removed. Channel 1 and 2 offset registers are sign magnitude coded. A negative number is applied to the Channel 1
offset register, CH1OS, for a negative offset adjustment. Note
that the Channel 2 offset register is inverted. A negative number
is applied to CH2OS for a positive offset adjustment. It is not
necessary to perform an offset correction in an energy measurement application if HPF in Channel 1 is switched on. Figure 33
shows the effect of offsets on the real power calculation. As seen
from Figure 33, an offset on Channel 1 and Channel 2 contributes
a dc component after multiplication. Because this dc component
is extracted by LPF2 to generate the active (real) power information, the offsets contribute an error to the active power
calculation. This problem is easily avoided by enabling HPF in
Channel 1. By removing the offset from at least one channel, no
error component is generated at dc by the multiplication. Error
terms at cos(ωt) are removed by LPF2 and by integration of the
active power signal in the active energy register (AENERGY[23:0])
—see the Energy Calculation section.
Rev. A | Page 15 of 60
Page 16
ADE7753
V
DC COMPONENT (INCLUDING ERROR TERM)
IS EXTRACTED BY THE LPF FOR REAL
× I
OS
OS
V × I
2
0
Figure 33. Effect of Channel Offsets on the Real Power Calculation
POWER CALCULATION
× V
I
OS
× I
V
OS
2ωω
FREQUENCY (RAD/S)
02875-0-033
di/dt CURRENT SENSOR AND
DIGITAL INTEGRATOR
A di/dt sensor detects changes in magnetic field caused by ac
current. Figure 35 shows the principle of a di/dt current sensor.
MAGNETIC FIELD CREATED BY CURRENT
(DIRECTLY PROPORTIONAL TO CURRENT)
The contents of the offset correction registers are 6-bit, sign and
magnitude coded. The weight of the LSB depends on the gain
setting, i.e., 1, 2, 4, 8, or 16. Table 6 shows the correctable offset
span for each of the gain settings and the LSB weight (mV) for
the offset correction registers. The maximum value that can be
written to the offset correction registers is ±31d—see Figure 34.
Figure 34 shows the relationship between the offset correction
register contents and the offset (mV) on the analog inputs for a
gain setting of 1. In order to perform an offset adjustment, the
analog inputs should be first connected to AGND, and there
should be no signal on either Channel 1 or Channel 2. A read
from Channel 1 or Channel 2 using the waveform register
indicates the offset in the channel. This offset can be canceled
by writing an equal and opposite offset value to the Channel 1
offset register, or an equal value to the Channel 2 offset register.
The offset correction can be confirmed by performing another
read. Note when adjusting the offset of Channel 1, one should
disable the digital integrator and the HPF.
Table 6. Offset Correction Range—Channels 1 and 2
Gain Correctable Span LSB Size
1 ±50 mV 1.61 mV/LSB
2 ±37 mV 1.19 mV/LSB
4 ±30 mV 0.97 mV/LSB
8 ±26 mV 0.84 mV/LSB
16 ±24 mV 0.77 mV/LSB
CH1OS[5:0]
+ EMF (ELECTROMOTIVE FORCE)
– INDUCED BY CHANGES IN
MAGNETIC FLUX DENSITY (di/dt)
02875-0-035
Figure 35. Principle of a di/dt Current Sensor
The flux density of a magnetic field induced by a current is
directly proportional to the magnitude of the current. The
changes in the magnetic flux density passing through a
conductor loop generate an electromotive force (EMF) between
the two ends of the loop. The EMF is a voltage signal, which is
proportional to the di/dt of the current. The voltage output
from the di/dt current sensor is determined by the mutual
inductance between the current-carrying conductor and the
di/dt sensor. The current signal needs to be recovered from the
di/dt signal before it can be used. An integrator is therefore
necessary to restore the signal to its original form. The ADE7753
has a built-in digital integrator to recover the current signal
from the di/dt sensor. The digital integrator on Channel 1 is
switched off by default when the ADE7753 is powered up.
Setting the MSB of CH1OS register turns on the integrator.
Figure 36 to Figure 39 show the magnitude and phase response
of the digital integrator.
10
0
–10
01,1111b
0x1F
0x00
0x3F
0mV
11,1111b
–50mV
Figure 34. Channel 1 Offset Correction Range (Gain = 1)
SIGN + 5 BITS
+50mV
OFFSET
ADJUST
SIGN + 5 BITS
02875-0-034
–20
GAIN (dB)
–30
–40
–50
2
10
FREQUENCY (Hz)
3
10
02875-0-036
Figure 36. Combined Gain Response of the
Digital Integrator and Phase Compensator
The current and voltage rms offsets can be adjusted with the
IRMSOS and VRMSOS registers—see Channel 1 RMS Offset
Compensation and Channel 2 RMS Offset Compensation
sections.
Rev. A | Page 16 of 60
Page 17
ADE7753
×
V
–88.0
–88.5
–89.0
–89.5
PHASE (Degrees)
–90.0
Note that the integrator has a –20 dB/dec attenuation and an
approximately –90° phase shift. When combined with a di/dt
sensor, the resulting magnitude and phase response should be a
flat gain over the frequency band of interest. The di/dt sensor
has a 20 dB/dec gain associated with it. It also generates significant high frequency noise, therefore a more effective antialiasing filter is needed to avoid noise due to aliasing—see the
Antialias Filter section.
When the digital integrator is switched off, the ADE7753 can be
used directly with a conventional current sensor such as a current
transformer (CT) or with a low resistance current shunt.
–90.5
2
10
FREQUENCY (Hz)
FREQ
3
10
Figure 37. Combined Phase Response of the
Digital Integrator and Phase Compensator
–1.0
–1.5
–2.0
–2.5
–3.0
–3.5
GAIN (dB)
–4.0
–4.5
–5.0
–5.5
–6.0
407045
50556065
FREQUENCY (Hz)
Figure 38. Combined Gain Response of the
Digital Integrator and Phase Compensator (40 Hz to 70 Hz)
–89.70
–89.75
02875-0-037
02875-0-038
ZERO-CROSSING DETECTION
The ADE7753 has a zero-crossing detection circuit on
Channel 2. This zero crossing is used to produce an external
zero-crossing signal (ZX), and it is also used in the calibration
mode—see the Calibrating an Energy Meter Based on the
ADE7753 section. The zero-crossing signal is also used to
initiate a temperature measurement on the ADE7753—see the
Temperature Measurement section.
Figure 40 shows how the zero-crossing signal is generated from
the output of LPF1.
1,×2,×1,
×8,×
V2P
2
V2N
1.0
0.93
16
{GAIN [7:5]}
PGA2
REFERENCE
ADC 2
f
–
2.32° @ 60Hz
LPF1
= 140Hz
3dB
–63%TO +63% FS
1
ZERO
CROSS
ZX
TO
MULTIPL IER
ZX
–89.80
–89.85
–89.90
–89.95
PHASE (Degrees)
–90.00
–90.05
40457050556065
FREQUENCY (Hz)
Figure 39. Combined Phase Response of the
Digital Integrator and Phase Compensator (40 Hz to 70 Hz)
02875-0-039
V2
Figure 40. Zero-Crossing Detection on Channel 2
The ZX signal goes logic high on a positive-going zero crossing
and logic low on a negative-going zero crossing on Channel 2.
The zero-crossing signal ZX is generated from the output of
LPF1. LPF1 has a single pole at 140 Hz (at CLKIN = 3.579545
MHz). As a result, there is a phase lag between the analog input
signal V2 and the output of LPF1. The phase response of this
filter is shown in the Channel 2 Sampling section. The phase lag
response of LPF1 results in a time delay of approximately
1.14 ms (@ 60 Hz) between the zero crossing on the analog
inputs of Channel 2 and the rising or falling edge of ZX.
LPF1
02875-0-040
Rev. A | Page 17 of 60
Page 18
ADE7753
The zero-crossing detection also drives the ZX flag in the
IRQ
interrupt status register. An active low in the
appears if the corresponding bit in the interrupt enable register
is set to Logic 1.
The flag in the interrupt status register as well as the
are reset to their default values when the interrupt status register with reset (RSTSTATUS) is read.
Zero-Crossing Timeout
The zero-crossing detection also has an associated timeout
register, ZXTOUT. This unsigned, 12-bit register is decremented
(1 LSB) every 128/CLKIN seconds. The register is reset to its
user programmed full-scale value every time a zero crossing is
detected on Channel 2. The default power on value in this
register is 0xFFF. If the internal register decrements to 0 before a
zero crossing is detected and the DISSAG bit in the mode
SAG
register is Logic 0, the
zero crossing is also indicated on the
pin goes active low. The absence of a
IRQ
enable bit in the interrupt enable register is set to Logic 1.
Irrespective of the enable bit setting, the ZXTO flag in the
interrupt status register is always set when the internal
ZXTOUT register is decremented to 0—see the ADE7753
Interrupts section.
The ZXOUT register can be written/read by the user and has an
address of 1Dh—see the ADE7753 Serial Interface section. The
resolution of the register is 128/CLKIN seconds per LSB. Thus
the maximum delay for an interrupt is 0.15 second (128/CLKIN
12
).
× 2
Figure 41 shows the mechanism of the zero-crossing timeout
detection when the line voltage stays at a fixed dc level for more
than CLKIN/128 × ZXTOUT seconds.
output also
IRQ
pin if the ZXTO
output
The resolution of this register is 2.2 ms/LSB when CLKIN =
3.579545 MHz, which represents 0.013% when the line frequency is 60 Hz. When the line frequency is 60 Hz, the value of
the period register is approximately 7576d. The length of the
register enables the measurement of line frequencies as low as
13.9 Hz.
The period register is stable at ±1 LSB when the line is
established and the measurement does not change. A settling
time of 1.8 seconds is associated with this filter before the
measurement is stable.
POWER SUPPLY MONITOR
The ADE7753 also contains an on-chip power supply monitor.
The analog supply (AVDD) is continuously monitored by the
ADE7753. If the supply is less than 4 V ± 5%, then the ADE7753
goes into an inactive state, that is, no energy is accumulated
when the supply voltage is below 4 V. This is useful to ensure
correct device operation at power-up and during power-down.
The power supply monitor has built-in hysteresis and filtering,
which give a high degree of immunity to false triggering due to
noisy supplies.
AV
DD
5V
4V
0V
ADE7753
POWER-ON
INACTIVE
STATE
INACTIVE
TIME
ACTIVEINACTIVE
12-BIT INTERNAL
REGISTER VALUE
ZXTOUT
CHANNEL 2
ZXTO
DETECTION
BIT
Figure 41. Zero-Crossing Timeout Detection
02875-0-041
PERIOD MEASUREMENT
The ADE7753 also provides the period measurement of the line.
The period register is an unsigned 16-bit register and is updated
every period. The MSB of this register is always zero.
Rev. A | Page 18 of 60
SAG
02875-0-042
Figure 42. On-Chip Power Supply Monitor
As seen in Figure 42, the trigger level is nominally set at 4 V. The
SAG
tolerance on this trigger level is about ±5%. The
pin can
also be used as a power supply monitor input to the MCU. The
SAG
pin goes logic low when the ADE7753 is in its inactive
state. The power supply and decoupling for the part should be
such that the ripple at AVDD does not exceed 5 V ±5%, as
specified for normal operation.
LINE VOLTAGE SAG DETECTION
In addition to the detection of the loss of the line voltage signal
(zero crossing), the ADE7753 can also be programmed to detect
when the absolute value of the line voltage drops below a
certain peak value for a number of line cycles. This condition is
illustrated in Figure 43.
Page 19
ADE7753
A
)
FULL SCALE
GLVL [7:0]
S
SAG
CHANNEL 2
SAGCYC [7:0] = 0x04
3 LINE CYCLES
Figure 43. ADE7753 Sag Detection
SAG RESET HIGH
WHEN CHANNEL 2
EXCEEDS SAGLVL [7:0]
02875-0-043
Figure 43 shows the line voltage falling below a threshold that is
set in the sag level register (SAGLVL[7:0]) for three line cycles.
The quantities 0 and 1 are not valid for the SAGCYC register,
and the contents represent one more than the desired number
of full line cycles. For example, when the sag cycle (SAGCYC[7:0])
SAG
contains 0x04, the
pin goes active low at the end of the
third line cycle for which the line voltage (Channel 2 signal)
falls below the threshold, if the DISSAG bit in the mode register
is Logic 0. As is the case when zero crossings are no longer
detected, the sag event is also recorded by setting the SAG flag
in the interrupt status register. If the SAG enable bit is set to
IRQ
Logic 1, the
Interrupts section. The
logic output goes active low—see the ADE7753
SAG
pin goes logic high again when the
absolute value of the signal on Channel 2 exceeds the sag level
set in the sag level register. This is shown in Figure 43 when the
SAG
pin goes high again during the fifth line cycle from the
time when the signal on Channel 2 first dropped below the
threshold level.
Sag Level Set
The contents of the sag level register (1 byte) are compared to
the absolute value of the most significant byte output from LPF1
after it is shifted left by one bit, thus, for example, the nominal
maximum code from LPF1 with a full-scale signal on Channel 2
is 0x2518—see the Channel 2 Sampling section. Shifting one bit
left gives 0x4A30. Therefore writing 0x4A to the SAG level
register puts the sag detection level at full scale. Writing 0x00 or
0x01 puts the sag detection level at 0. The SAG level register is
compared to the most significant byte of a waveform sample
after the shift left and detection is made when the contents of
the sag level register are greater.
PEAK DETECTION
The ADE7753 can also be programmed to detect when the
absolute value of the voltage or current channel exceeds a
specified peak value. Figure 44 illustrates the behavior of the
peak detection for the voltage channel. Both Channel 1 and
Channel 2 are monitored at the same time.
V
2
VPKLVL[7:0]
PKV RESET LOW
WHEN RSTSTATUS
REGISTER IS READ
PKV INTERRUPT
FLAG (BIT 8 OF
STATUS REGISTER
READ RSTSTATUS
REGISTER
Figure 44. ADE7753 Peak Level Detection
02875-0-088
Figure 44 shows a line voltage exceeding a threshold that is set
in the voltage peak register (VPKLVL[7:0]). The voltage peak
event is recorded by setting the PKV flag in the interrupt status
register. If the PKV enable bit is set to Logic 1 in the interrupt
mask register, the
IRQ
logic output goes active low. Similarly, the
current peak event is recorded by setting the PKI flag in the
interrupt status register—see the ADE7753 Interrupts section.
Peak Level Set
The contents of the VPKLVL and IPKLVL registers are
respectively compared to the absolute value of Channel 1 and
Channel 2 after they are multiplied by 2. Thus, for example, the
nominal maximum code from the Channel 1 ADC with a fullscale signal is 0x2851EC—see the Channel 1 Sampling section.
Multiplying by 2 gives 0x50A3D8. Therefore, writing 0x50 to
the IPKLVL register, for example, puts the Channel 1 peak
detection level at full scale and sets the current peak detection
to its least sensitive value. Writing 0x00 puts the Channel 1
detection level at 0. The detection is done by comparing the
contents of the IPKLVL register to the incoming Channel 1
IRQ
sample. The
pin indicates that the peak level is exceeded if
the PKI or PKV bits are set in the interrupt enable register
(IRQEN[15:0]) at Address 0x0A.
Peak Level Record
The ADE7753 records the maximum absolute value reached by
Channel 1 and Channel 2 in two different registers—IPEAK
and VPEAK, respectively. VPEAK and IPEAK are 24-bit unsigned
registers. These registers are updated each time the absolute
value of the waveform sample from the corresponding channel
is above the value stored in the VPEAK or IPEAK register. The
contents of the VPEAK register correspond to 2× the maximum
absolute value observed on the Channel 2 input. The contents of
IPEAK represent the maximum absolute value observed on the
Channel 1 input. Reading the RSTVPEAK and RSTIPEAK
registers clears their respective contents after the read operation.
Rev. A | Page 19 of 60
Page 20
ADE7753
ADE7753 INTERRUPTS
ADE7753 interrupts are managed through the interrupt status
register (STATUS[15:0]) and the interrupt enable register
(IRQEN[15:0]). When an interrupt event occurs in the ADE7753,
the corresponding flag in the status register is set to Logic 1—
see the Interrupt Status Register section. If the enable bit for this
interrupt in the interrupt enable register is Logic 1, then the
IRQ
logic output goes active low. The flag bits in the status
register are set irrespective of the state of the enable bits.
To determine the source of the interrupt, the system master
(MCU) should perform a read from the status register with
reset (RSTSTATUS[15:0]). This is achieved by carrying out a
IRQ
read from Address 0x0C. The
completion of the interrupt status register read command—see
the Interrupt Timing section. When carrying out a read with
reset, the ADE7753 is designed to ensure that no interrupt
events are missed. If an interrupt event occurs just as the status
register is being read, the event is not lost and the
output is guaranteed to go high for the duration of the interrupt
status register data transfer before going logic low again to
indicate the pending interrupt. See the next section for a more
detailed description.
IRQ
output goes logic high on
t
1
IRQ
logic
Using the ADE7753 Interrupts with an MCU
Figure 46 shows a timing diagram with a suggested implementation of ADE7753 interrupt management using an MCU. At
IRQ
, the line goes active low indicating that one or more
time t
1
IRQ
interrupt events have occurred in the ADE7753. The
logic
output should be tied to a negative edge-triggered external
interrupt on the MCU. On detection of the negative edge, the
MCU should be configured to start executing its interrupt
service routine (ISR). On entering the ISR, all interrupts should
be disabled by using the global interrupt enable bit. At this
point, the MCU external interrupt flag can be cleared to capture
interrupt events that occur during the current ISR. When the
MCU interrupt flag is cleared, a read from the status register
IRQ
with reset is carried out. This causes the
logic high (t
)—see the Interrupt Timing section. The status
2
line to be reset
register contents are used to determine the source of the
interrupt(s) and therefore the appropriate action to be taken. If
a subsequent interrupt event occurs during the ISR, that event is
recorded by the MCU external interrupt flag being set again (t
).
3
On returning from the ISR, the global interrupt mask is cleared
(same instruction cycle), and the external interrupt flag causes
the MCU to jump to its ISR once a gain. This ensures that the
MCU does not miss any external interrupts.
MCU
INTERRUPT
t
2
t
3
FLAG SET
MCU
PROGRAM
SEQUENCE
CS
SCLK
DIN
DOUT
IRQ
JUMP
ISR
GLOBAL
INTERRUPT
TO
MASK SET
CLEAR MCU
INTERRUPT
FLAG
READ
STATUS WITH
RESET (0x05)
Figure 45. ADE7753 Interrupt Management
t
1
00000101
READ STATUS REGISTER COMMAND
Figure 46. ADE7753 Interrupt Timing
ISR ACTION
(BASED ON STATUS CONTENTS)
t
9
t
11
DB7DB7DB0
ISR RETURN
GLOBAL INTERRUPT
MASK RESET
t
11
STATUS REGISTER CONTENTS
DB0
02875-0-045
JUMP
TO
ISR
02875-0-044
Rev. A | Page 20 of 60
Page 21
ADE7753
S
S
Interrupt Timing
The ADE7753 Serial Interface section should be reviewed first
before reviewing the interrupt timing. As previously described,
IRQ
when the
output goes low, the MCU ISR must read the
interrupt status register to determine the source of the interrupt.
When reading the status register contents, the
IRQ
output is set
high on the last falling edge of SCLK of the first byte transfer
(read interrupt status register command). The
IRQ
output is
held high until the last bit of the next 15-bit transfer is shifted
out (interrupt status register contents)—see Figure 45. If an
interrupt is pending at this time, the
If no interrupt is pending, the
IRQ
output goes low again.
IRQ
output stays high.
TEMPERATURE MEASUREMENT
The ADE7753 also includes an on-chip temperature sensor. A
temperature measurement can be made by setting Bit 5 in the
mode register. When Bit 5 is set logic high in the mode register,
the ADE7753 initiates a temperature measurement on the next
zero crossing. When the zero crossing on Channel 2 is detected,
the voltage output from the temperature sensing circuit is
connected to ADC1 (Channel 1) for digitizing. The resulting
code is processed and placed in the temperature register
(TEMP[7:0]) approximately 26 µs later (24 CLKIN cycles). If
IRQ
enabled in the interrupt enable register (Bit 5), the
output
goes active low when the temperature conversion is finished.
The contents of the temperature register are signed (twos
complement) with a resolution of approximately 1.5 LSB/°C.
The temperature register produces a code of 0x00 when the
ambient temperature is approximately −25°C. The temperature
measurement is uncalibrated in the ADE7753 and has an offset
tolerance as high as ±25°C.
ADE7753 ANALOG-TO-DIGITAL CONVERSION
The analog-to-digital conversion in the ADE7753 is carried out
using two second-order Σ-∆ ADCs. For simplicity, the block
diagram in Figure 47 shows a first-order Σ-∆ ADC. The
converter is made up of the Σ-∆ modulator and the digital lowpass filter.
V
REF
1-BIT DAC
MCLK/4
LATCHED
COMPARATOR
+
–
.....10100101.....
Σ
-∆ ADC
02875-0-046
DIGITAL
LOW-PASS
FILTER
24
ANALOG
LOW-PASS FILTER
R
C
INTEGRATOR
+
–
Figure 47. First-Order
A Σ-∆ modulator converts the input signal into a continuous
serial stream of 1s and 0s at a rate determined by the sampling
clock. In the ADE7753, the sampling clock is equal to CLKIN/4.
The 1-bit DAC in the feedback loop is driven by the serial data
stream. The DAC output is subtracted from the input signal. If
the loop gain is high enough, the average value of the DAC output (and therefore the bit stream) can approach that of the input
signal level. For any given input value in a single sampling interval,
the data from the 1-bit ADC is virtually meaningless. Only when
a large number of samples are averaged is a meaningful result
obtained. This averaging is carried out in the second part of the
ADC, the digital low-pass filter. By averaging a large number of
bits from the modulator, the low-pass filter can produce 24-bit
data-words that are proportional to the input signal level.
The Σ-∆ converter uses two techniques to achieve high
resolution from what is essentially a 1-bit conversion technique.
The first is oversampling. Oversampling means that the signal is
sampled at a rate (frequency), which is many times higher than
the bandwidth of interest. For example, the sampling rate in the
ADE7753 is CLKIN/4 (894 kHz) and the band of interest is
40 Hz to 2 kHz. Oversampling has the effect of spreading the
quantization noise (noise due to sampling) over a wider
bandwidth. With the noise spread more thinly over a wider
bandwidth, the quantization noise in the band of interest is
lowered—see Figure 48. However, oversampling alone is not
efficient enough to improve the signal-to-noise ratio (SNR) in
the band of interest. For example, an oversampling ratio of 4 is
required just to increase the SNR by only 6 dB (1 bit). To keep
the oversampling ratio at a reasonable level, it is possible to
shape the quantization noise so that the majority of the noise
lies at the higher frequencies. In the Σ-∆ modulator, the noise is
shaped by the integrator, which has a high-pass-type response
for the quantization noise. The result is that most of the noise is
at the higher frequencies where it can be removed by the digital
low-pass filter. This noise shaping is shown in Figure 48.
ANTILALIAS
FILTER (RC)
IGNAL
NOISE
IGNAL
NOISE
DIGITAL
FILTER
FREQUENCY (kHz)
HIGH RESOLUTION
OUTPUT FROM DIGITAL
LPF
FREQUENCY (kHz)
Figure 48. Noise Reduction Due to Oversampling and
Noise Shaping in the Analog Modulator
SHAPED
44708942
44708942
NOISE
SAMPLING
FREQUENCY
02875-0-047
Rev. A | Page 21 of 60
Page 22
ADE7753
Antialias Filter
Figure 47 also shows an analog low-pass filter (RC) on the input
to the modulator. This filter is present to prevent aliasing.
Aliasing is an artifact of all sampled systems. Aliasing means
that frequency components in the input signal to the ADC,
which are higher than half the sampling rate of the ADC,
appear in the sampled signal at a frequency below half the
sampling rate. Figure 49 illustrates the effect. Frequency
components (arrows shown in black) above half the sampling
frequency (also know as the Nyquist frequency, i.e., 447 kHz)
are imaged or folded back down below 447 kHz. This happens
with all ADCs regardless of the architecture. In the example
shown, only frequencies near the sampling frequency, i.e.,
894 kHz, move into the band of interest for metering, i.e., 40 Hz
to 2 kHz. This allows the use of a very simple LPF (low-pass
filter) to attenuate high frequency (near 900 kHz) noise, and
prevents distortion in the band of interest. For conventional
current sensors, a simple RC filter (single-pole LPF) with a
corner frequency of 10 kHz produces an attenuation of
approximately 40 dB at 894 kHz—see Figure 49. The 20 dB per
decade attenuation is usually sufficient to eliminate the effects
of aliasing for conventional current sensors. However, for a di/dt
sensor such as a Rogowski coil, the sensor has a 20 dB per
decade gain. This neutralizes the –20 dB per decade attenuation
produced by one simple LPF. Therefore, when using a di/dt
sensor, care should be taken to offset the 20 dB per decade gain.
One simple approach is to cascade two RC filters to produce the
–40 dB per decade attenuation needed.
ALIASING EFFECTS
ADE7753 Reference Circuit
Figure 50 shows a simplified version of the reference output
circuitry. The nominal reference voltage at the REF
IN/OUT
pin is
2.42 V. This is the reference voltage used for the ADCs in the
ADE7753. However, Channel 1 has three input range selections
that are selected by dividing down the reference value used for
the ADC in Channel 1. The reference value used for Channel 1
is divided down to ½ and ¼ of the nominal value by using an
internal resistor divider, as shown in Figure 50.
OUTPUT
IMPEDANCE
6kΩ
REF
IN/OUT
2.42V
REFERENCE INPUT
TO ADC CHANNEL 1
(RANGE SELECT)
2.42V, 1.21V, 0.6V
02875-0-049
The REF
MAXIMUM
LOAD = 10µA
PTAT
60µA
Figure 50. ADE7753 Reference Circuit Output
pin can be overdriven by an external source, for
IN/OUT
2.5V
1.7kΩ
12.5kΩ
12.5kΩ
12.5kΩ
12.5kΩ
example, an external 2.5 V reference. Note that the nominal
reference value supplied to the ADCs is now 2.5 V, not 2.42 V,
which has the effect of increasing the nominal analog input
signal range by 2.5/2.42 × 100% = 3% or from 0.5 V to 0.5165 V.
SAMPLING
IMAGE
FREQUENCIES
02447894
Figure 49. ADC and Signal Processing in Channel 1 Outline Dimensions
FREQUENCY (kHz)
FREQUENCY
02875-0-048
ADC Transfer Function
The following expression relates the output of the LPF in the
Σ-∆ ADC to the analog input signal level. Both ADCs in the
ADE7753 are designed to produce the same output code for the
same input signal level.
V
() 3.0492262,144
Code ADCV=××
IN
OUT
(1)
Therefore with a full-scale signal on the input of 0.5 V and an
internal reference of 2.42 V, the ADC output code is nominally
165,151 or 2851Fh. The maximum code from the ADC is
±262,144; this is equivalent to an input signal level of ±0.794 V.
However, for specified performance, it is recommended that the
full-scale input signal level of 0.5 V not be exceeded.
The voltage of the ADE7753 reference drifts slightly with
temperature—see the ADE7753 Specifications for the
temperature coefficient specification (in ppm/°C). The value of
the temperature drift varies from part to part. Since the
reference is used for the ADCs in both Channels 1 and 2, any
x% drift in the reference results in 2×% deviation of the meter
accuracy. The reference drift resulting from temperature
changes is usually very small and it is typically much smaller
than the drift of other components on a meter. However, if
guaranteed temperature performance is needed, one needs to
use an external voltage reference. Alternatively, the meter can be
calibrated at multiple temperatures. Real-time compensation
can be achieved easily by using the on-chip temperature sensor.
CHANNEL 1 ADC
Figure 51 shows the ADC and signal processing chain for
Channel 1. In waveform sampling mode, the ADC outputs a
signed twos complement 24-bit data-word at a maximum of
27.9 kSPS (CLKIN/128). With the specified full-scale analog
input signal of 0.5 V (or 0.25 V or 0.125 V—see the Analog
Inputs section) the ADC produces an output code that is
approximately between 0x2851EC (+2,642,412d) and
0xD7AE14 (–2,642,412d)—see Figure 51.
Rev. A | Page 22 of 60
Page 23
ADE7753
0.5V, 0.25V,
0.125V, 62.5mV,
31.3mV, 15.6mV,
2.42V, 1.21V, 0.6V
×1, ×2, ×4,
×8, ×16
{GAIN[2:0]}
V1P
PGA1
V1
V1N
V1
0V
ANALOG
INPUT
RANGE
*WHEN DIGITAL INTEGRATOR IS ENABLED, FULL-SCALE OUTPUT DATA IS ATTENUATED
DEPENDING ON THE SIGNAL FREQUENCY BECAUSE THE INTEGRATOR HAS A –20dB/DECADE
FREQUENCY RESPONSE. WHEN DISABLED, THE OUTPUT WILL NOT BE FURTHER ATTENUATED.
0x2851EC
0x00000
0xD7AE4
REFERENCE
ADC 1
ADC OUTPUT
WORD RANGE
Figure 51. ADC and Signal Processing in Channel 1
{GAIN[4:3]}
HPF
0x2851EC
0x000000
0xD7AE4
DIGITAL
INTEGRATOR*
dt
CHANNEL 1
(CURRENT WAVEFORM)
DATA RANGE
CURRENT RMS (IRMS)
CALCULATION
WAVEFORM SAMPLE
REGISTER
ACTIVE AND REACTIVE
POWER CALCULATION
CHANNEL 1
50Hz
0x1EF73C
0x000000
0xEI08C4
60Hz
0x19CE08
0x000000
0xE631F8
(CURRENT WAVEFORM)
DATA RANGE AFTER
INTEGRATOR (50Hz)
CHANNEL 1
(CURRENT WAVEFORM)
DATA RANGE AFTER
INTEGRATOR (60Hz)
02875-0-052
Channel 1 Sampling
The waveform samples can also be routed to the waveform
register (MODE[14:13] = 1,0) to be read by the system master
(MCU). In waveform sampling mode, the WSMP bit (Bit 3) in
the interrupt enable register must also be set to Logic 1. The
active, apparent power, and energy calculation remain
uninterrupted during waveform sampling.
When in waveform sampling mode, one of four output sample
rates can be chosen by using Bits 11 and 12 of the mode register
(WAVSEL1,0). The output sample rate can be 27.9 kSPS, 14 kSPS,
7 kSPS, or 3.5 kSPS—see the Mode Register (0X09) section. The
IRQ
interrupt request output,
, signals a new sample availability
by going active low. The timing is shown in Figure 52. The 24-bit
waveform samples are transferred from the ADE7753 one byte
(eight bits) at a time, with the most significant byte shifted out
first. The 24-bit data-word is right justified—see the ADE7753
IRQ
Serial Interface section. The interrupt request output
stays
low until the interrupt routine reads the reset status register—
see the ADE7753 Interrupts section.
IRQ
SCLK
READ FROM WAVEFORM
0 0 01 HEX
DIN
DOUT
0
SIGN
CHANNEL 1 DATA
(24 BITS)
Figure 52. Waveform Sampling Channel 1
02875-0-050
Channel 1 RMS Calculation
Root mean square (rms) value of a continuous signal V(t) is
defined as
T
1
2
VRMS =
V
rms
×=
T
dttV
)(
∫
0
(2)
For time sampling signals, rms calculation involves squaring the
signal, taking the average and obtaining the square root:
N
VRMS =
V
rms
1
N
2
×=
∑
i
=
1
(3)
iV
)(
The ADE7753 simultaneously calculates the rms values for
Channel 1 and Channel 2 in different registers. Figure 53 shows
the detail of the signal processing chain for the rms calculation
on Channel 1. The Channel 1 rms value is processed from the
samples used in the Channel 1 waveform sampling mode. The
Channel 1 rms value is stored in an unsigned 24-bit register
(IRMS). One LSB of the Channel 1 rms register is equivalent to
one LSB of a Channel 1 waveform sample. The update rate of
the Channel 1 rms measurement is CLKIN/4.
Rev. A | Page 23 of 60
Page 24
ADE7753
CURRENT SIGNAL (i(t))
0x2851EC
0x00
0xD7AE14
CHANNEL 1
2424
Figure 53. Channel 1 RMS Signal Processing
With the specified full-scale analog input signal of 0.5 V, the
ADC produces an output code that is approximately
±2,642,412d—see the Channel 1 ADC section. The equivalent
rms value of a full-scale ac signal are 1,868,467d (0x1C82B3).
The current rms measurement provided in the ADE7753 is
accurate to within 1% for signal input between full scale and full
scale/100. The conversion from the register value to amps must
be done externally in the microprocessor using an amps/LSB
constant. To minimize noise, synchronize the reading of the rms
register with the zero crossing of the voltage input and take the
average of a number of readings.
Channel 1 RMS Offset Compensation
The ADE7753 incorporates a Channel 1 rms offset compensation register (IRMSOS). This is a 12-bit signed register that can
be used to remove offset in the Channel 1 rms calculation. An
offset could exist in the rms calculation due to input noises that
2
are integrated in the dc component of V
(t). The offset
calibration allows the content of the IRMS register to be
maintained at 0 when no input is present on Channel 1.
One LSB of the Channel 1 rms offset is equivalent to 32,768 LSB
of the square of the Channel 1 rms register. Assuming that the
maximum value from the Channel 1 rms calculation is
1,868,467d with full-scale ac inputs, then 1 LSB of the Channel 1
rms offset represents 0.46% of measurement error at –60 dB
down of full scale.
32768
IRMS =
where IRMS
0
is the rms measurement without offset correction.
0
×+ IRMSOSIRMS (4)
To measure the offset of the rms measurement, two data points
are needed from non-zero input values, for example, the base
current, I
, and I
b
/100. The offset can be calculated from these
max
measurements.
IRMSOS[11:0]
26225
2
sgn2272172162
LPF3HPF1
+
15
0x1C82B3
0x00
I
RMS
(t)
IRMS
02875-0-0051
CHANNEL 2 ADC
Channel 2 Sampling
In Channel 2 waveform sampling mode (MODE[14:13] = 1,1
and WSMP = 1), the ADC output code scaling for Channel 2 is
not the same as Channel 1. The Channel 2 waveform sample is a
16-bit word and sign extended to 24 bits. For normal operation,
the differential voltage signal between V2P and V2N should not
exceed 0.5 V. With maximum voltage input (±0.5 V at PGA gain
of 1), the output from the ADC swings between 0x2852 and
0xD7AE (±10,322d). However, before being passed to the waveform register, the ADC output is passed through a single-pole,
low-pass filter with a cutoff frequency of 140 Hz. The plots in
Figure 54 show the magnitude and phase response of this filter.
0
–10
–20
50Hz, –19.7°
–30
–40
–50
PHASE (Degrees)
–60
–70
–80
–90
1
10
Figure 54. Magnitude and Phase Response of LPF1
50Hz, –0.52dB
60Hz, –23.2°
FREQUENCY (Hz)
The LPF1 has the effect of attenuating the signal. For example,
if the line frequency is 60 Hz, then the signal at the output of
LPF1 is attenuated by about 8%.
=
fH73.0919.0
)(
1
⎛
Hz
60
⎜
+
1
⎜
Hz
140
⎝
10
2
⎞
⎟
⎟
⎠
60Hz, –0.73dB
2
dB
−==
(5)
0
–2
–4
–6
–8
–10
–12
–14
–16
–18
3
10
02875-0-053
GAIN (dB)
Note LPF1 does not affect the active power calculation. The
signal processing chain in Channel 2 is illustrated in Figure 55.
Rev. A | Page 24 of 60
Page 25
ADE7753
V2P
V2
V2N
ANALOG
INPUT RANGE
0.5V, 0.25, 0.125,
62.5mV, 31.25mV
0V
×1, ×2, ×4,
×8, ×16
PGA2
V1
{GAIN [7:5]}
REFERENCE
ADC 2
Figure 55. ADC and Signal Processing in Channel 2
VOLTAGE SIGNAL (V(t))
0x2518
0x0
0xDAE8
CHANNEL 2
Figure 56. Channel 2 RMS Signal Processing
Channel 2 has only one analog input range (0.5 V differential).
Like Channel 1, Channel 2 has a PGA with gain selections of 1,
2, 4, 8, and 16. For energy measurement, the output of the ADC
is passed directly to the multiplier and is not filtered. An HPF is
not required to remove any dc offset since it is only required to
remove the offset from one channel to eliminate errors due to
offsets in the power calculation. When in waveform sampling
mode, one of four output sample rates can be chosen by using
Bits 11 and 12 of the mode register. The available output sample
rates are 27.9 kSPS, 14 kSPS, 7 kSPS, or 3.5 kSPS—see the Mode
IRQ
Register (0x09) section. The interrupt request output
signals that a sample is available by going active low. The timing
is the same as that for Channel 1, as shown in Figure 52.
Channel 2 RMS Calculation
Figure 56 shows the details of the signal processing chain for
the rms calculation on Channel 2. The Channel 2 rms value is
processed from the samples used in the Channel 2 waveform
sampling mode. The rms value is slightly attenuated because of
LPF1. Channel 2 rms value is stored in the unsigned 24-bit
VRMS register. The update rate of the Channel 2 rms
measurement is CLKIN/4.
With the specified full-scale ac analog input signal of 0.5 V, the
output from the LPF1 swings between 0x2518 and 0xDAE8 at
60 Hz—see the Channel 2 ADC section. The equivalent rms
value of this full-scale ac signal is approximately 1,561,400
(0z17D338) in the VRMS register. The voltage rms measurement provided in the ADE7753 is accurate to within ±0.5% for
signal input between full scale and full scale/20. The conversion
2.42V
0xDAE8
0xD7AE
0x2852
0x2581
0x0000
LPF3LPF1
ACTIVE AND REACTIVE
LPF1
LPF OUTPUT
WORD RANGE
ENERGYCALCULATION
VRMS CALCULATIO N
AND WAVEFORM
SAMPLING
(PEAK/SAG/ZX )
02875-0-054
VRMOS[11:0]
9
sgn2822212
2
0
VRMS[23:0]
0x17D338
+
+
0x00
02875-0-0055
from the register value to volts must be done externally in the
microprocessor using a volts/LSB constant. Since the low-pass
filtering used for calculating the rms value is imperfect, there is
some ripple noise from 2
ω term present in the rms measure-
ment. To minimize the noise effect in the reading, synchronize
the rms reading with the zero crossings of the voltage input.
Channel 2 RMS Offset Compensation
The ADE7753 incorporates a Channel 2 rms offset compensation
register (VRMSOS). This is a 12-bit signed register that can be
used to remove offset in the Channel 2 rms calculation. An
offset could exist in the rms calculation due to input noises and
dc offset in the input samples. The offset calibration allows the
contents of the VRMS register to be maintained at 0 when no
voltage is applied. One LSB of the Channel 2 rms offset is
equivalent to one LSB of the rms register. Assuming that the
maximum value from the Channel 2 rms calculation is
1,561,400d with full-scale ac inputs, then one LSB of the
Channel 2 rms offset represents 0.064% of measurement
error at –60 dB down of full scale.
VRMS = VRMS
where VRMS
0
+ VRMSOS (6)
0
is the rms measurement without offset correction.
The voltage rms offset compensation should be done by testing
the rms results at two non-zero input levels. One measurement
can be done close to full scale and the other at approximately
full scale/10. The voltage offset compensation can be derived
from these measurements. If the voltage rms offset register does
not have enough range, the CH2OS register can also be used.
Rev. A | Page 25 of 60
Page 26
ADE7753
V
V
PHASE COMPENSATION
When the HPF is disabled, the phase error between Channel 1
and Channel 2 is 0 from dc to 3.5 kHz. When HPF is enabled,
Channel 1 has the phase response illustrated in Figure 58 and
Figure 59. Also shown in Figure 60 is the magnitude response of
the filter. As can be seen from the plots, the phase response is
almost 0 from 45 Hz to 1 kHz. This is all that is required in
typical energy measurement applications. However, despite
being internally phase compensated, the ADE7753 must work
with transducers, which could have inherent phase errors. For
example, a phase error of 0.1° to 0.3° is not uncommon for a
current transformer (CT). These phase errors can vary from
part to part, and they must be corrected in order to perform
accurate power calculations. The errors associated with phase
mismatch are particularly noticeable at low power factors. The
ADE7753 provides a means of digitally calibrating these small
phase errors. The ADE7753 allows a small time delay or time
advance to be introduced into the signal processing chain to
compensate for small phase errors. Because the compensation is
in time, this technique should be used only for small phase
errors in the range of 0.1° to 0.5°. Correcting large phase errors
using a time shift technique can introduce significant phase
errors at higher harmonics.
The phase calibration register (PHCAL[5:0]) is a twos complement signed single-byte register that has values ranging from
0x21 (–31d) to 0x1F (31d).
The register is centered at 0x0D, so that writing 0x0D to the
register gives 0 delay. By changing the PHCAL register, the time
delay in the Channel 2 signal path can change from –102.12 µs
to +39.96 µs (CLKIN = 3.579545 MHz). One LSB is equivalent
to 2.22 µs (CLKIN/8) time delay or advance. A line frequency of
60 Hz gives a phase resolution of 0.048° at the fundamental (i.e.,
360° × 2.22 µs × 60 Hz). Figure 57 illustrates how the phase
compensation is used to remove a 0.1° phase lead in Channel 1
due to the external transducer. To cancel the lead (0.1°) in
Channel 1, a phase lead must also be introduced into Channel 2.
The resolution of the phase adjustment allows the introduction
of a phase lead in increment of 0.048°. The phase lead is achieved
by introducing a time advance into Channel 2. A time advance
of 4.48 µs is made by writing −2 (0x0B) to the time delay block,
thus reducing the amount of time delay by 4.48 µs, or equivalently, a phase lead of approximately 0.1° at line frequency of
60 Hz. 0x0B represents –2 because the register is centered with 0
at 0x0D.
V1P
PGA1
1
V1N
V2P
PGA2
2
V2N
V1
ADC 1
1
ADC 2
V2
0.1°
60Hz
HPF
24
24
DELAY BLOCK
4.48µs/LSB
50
110100
PHCAL [5:0]
--100µs TO +34µs
CHANNEL 2 DELAY
REDUCED BY 4.48µs
(0.1°LEAD AT 60Hz)
0Bh IN PHCAL [5.0]
V2
V1
60Hz
LPF2
02875-0-056
Figure 57. Phase Calibration
0.9
0.8
0.7
0.6
0.5
0.4
0.3
PHASE (Degrees)
0.2
0.1
0
–0.1
2
10
FREQUENCY (Hz)
3
10
02875-0-057
4
10
Figure 58. Combined Phase Response of the HPF and
Phase Compensation (10 Hz to 1 kHz)
0.20
0.18
0.16
0.14
0.12
0.10
0.08
PHASE (Degrees)
0.06
0.04
0.02
0
40
455055606570
FREQUENCY (Hz)
02875-0-058
Figure 59. Combined Phase Response of the HPF and
Phase Compensation (40 Hz to 70 Hz)
Rev. A | Page 26 of 60
Page 27
ADE7753
0.4
0.3
0.2
0.1
0.0
ERROR (%)
–0.1
–0.2
–0.3
–0.4
54565860626466
FREQUENCY (Hz)
02875-0-059
Figure 60. Combined Gain Response of the HPF and Phase Compensation
ACTIVE POWER CALCULATION
Power is defined as the rate of energy flow from source to load.
It is defined as the product of the voltage and current waveforms. The resulting waveform is called the instantaneous
power signal and is equal to the rate of energy flow at every
instant of time. The unit of power is the watt or joules/sec.
Equation 9 gives an expression for the instantaneous power
signal in an ac system.
v(t) =
i(t) =
where:
V is the rms voltage.
I is the rms current.
)sin(2tVω× (7)
)sin(2tIω× (8)
The instantaneous power signal p(t) is generated by multiplying
the current and voltage signals. The dc component of the
instantaneous power signal is then extracted by LPF2 (low-pass
filter) to obtain the active power information. This process is
illustrated in Figure 61.
0x19999A
0xCCCCD
0x00000
INSTANTANEOUS
POWER SIGNAL
VI
CURRENT
i(t) = 2
×i×
sin(ωt)
VOLTAGE
×v×
v(t) = 2
Figure 61. Active Power Calculation
p(t) = v
sin(ωt)
×
i-v×i×cos(2ωt)
ACTIVE REAL POWER
×
SIGNAL= v
i
02875-0-060
Since LPF2 does not have an ideal “brick wall” frequency
response—see Figure 62, the active power signal has some
ripple due to the instantaneous power signal. This ripple is
sinusoidal and has a frequency equal to twice the line frequency.
Because the ripple is sinusoidal in nature, it is removed when
the active power signal is integrated to calculate energy—see the
Energy Calculation section.
0
–4
)()()(titvtp×=
)2cos()(tVIVItpω−= (9)
The average power over an integral number of line cycles (n) is
given by the expression in Equation 10.
P =
nT
1
∫
0
=nTVIdttp
)(
(10)
where:
T is the line cycle period.
P is referred to as the active or real power.
Note that the active power is equal to the dc component of the
instantaneous power signal p(t) in Equation 8, i.e., VI. This is
the relationship used to calculate active power in the ADE7753.
Rev. A | Page 27 of 60
–8
–12
dB
–16
–20
–24
1
31030100
FREQUENCY (Hz)
02875-0-061
Figure 62. Frequency Response of LPF2
Page 28
ADE7753
CURRENT
CHANNEL
VOLTAGE
CHANNEL
OUTPUT LPF2
T
APOS[15:0]
LPF2
ACTIVE POWER
SIGNAL
4
CLKIN
TIME (nT)
+
+
WGAIN[11:0]
WAVEFORM
REGISTER
VALUES
Figure 63. ADE7753 Active Energy Calculation
Figure 63 shows the signal processing chain for the active power
calculation in the ADE7753. As explained, the active power is
calculated by low-pass filtering the instantaneous power signal.
Note that when reading the waveform samples from the output
of LPF2, the gain of the active energy can be adjusted by using
the multiplier and watt gain register (WGAIN[11:0]). The gain
is adjusted by writing a twos complement 12-bit word to the
watt gain register. Equation 11 shows how the gain adjustment
is related to the contents of the watt gain register:
⎛
⎜
⎜
⎝
PowerActiveWGAINOutput
⎧
1
⎨
⎩
WGAIN
+×=
⎞
⎫
⎟
(11)
⎬
⎟
12
2
⎭
⎠
For example, when 0x7FF is written to the watt gain register, the
power output is scaled up by 50%. 0x7FF = 2047d, 2047/2
12
=
0.5. Similarly, 0x800 = –2048d (signed twos complement) and
power output is scaled by –50%. Each LSB scales the power
output by 0.0244%. Figure 64 shows the maximum code (in
hex) output range for the active power signal (LPF2). Note that
the output range changes depending on the contents of the watt
gain register. The minimum output range is given when the watt
gain register contents are equal to 0x800, and the maximum
range is given by writing 0x7FF to the watt gain register. This
can be used to calibrate the active power (or energy) calculation
in the ADE7753.
WDIV[7:0]
%
AENERGY [23:0]
230
480
OUTPUTS FROM THE LPF2 ARE
ACCUMULATED (INTEGRATED) IN
THE INTERNAL ACTIVE ENERGY REGISTER
0x13333
0xCCCD
0x6666
0x00000
0xF999A
0xF3333
ACTIVE POWER OUTPUT
0xECCCD
Figure 64. Active Power Calculation Output Range
UPPER 24 BITS ARE
ACCESSIBLETHROUGH
AENERGY[23:0] REGISTER
02875-0-063
0x0000x7FF0x800
{WGAIN[11:0]}
ACTIVE POWER
CALIBRATION RANGE
POSITIVE
POWER
NEGATIVE
POWER
ENERGY CALCULATION
As stated earlier, power is defined as the rate of energy flow.
This relationship can be expressed mathematically in Equation 12.
dE
P =
where:
P is power.
E is energy.
Conversely, energy is given as the integral of power.
(12)
dt
02875-0-062
= PdtE
(13)
∫
Rev. A | Page 28 of 60
Page 29
ADE7753
V
E
HPF
I
CURRENT SIGNAL – i(t)
MULTIPLIER
1
VOLTAGE SIGNAL– v(t)
INSTANTANEOUS
POWER SIGNAL – p(t)
0x19999A
0x000000
Figure 65. Active Power Signal Processing
LPF2
24
sgn252-62-72
The ADE7753 achieves the integration of the active power
signal by continuously accumulating the active power signal in
an internal nonreadable 49-bit energy register. The active
energy register (AENERGY[23:0]) represents the upper 24 bits
of this internal register. This discrete time accumulation or
summation is equivalent to integration in continuous time.
Equation 14 expresses the relationship.
∞
==×
()( )
ptdt LimpnT T
∫
⎧⎫
⎨
∑
0
t
→
1
n
=
⎩
(14)
⎬
⎭
where:
n is the discrete time sample number.
T is the sample period.
The discrete time sample period (T) for the accumulation
register in the ADE7753 is 1.1µs (4/CLKIN). As well as
calculating the energy, this integration removes any sinusoidal
components that might be in the active power signal. Figure 65
shows this discrete time integration or accumulation. The active
power signal in the waveform register is continuously added to
the internal active energy register. This addition is a signed
addition; therefore negative energy is subtracted from the active
energy contents. The exception to this is when POAM is
selected in the MODE[15:0] register. In this case, only positive
energy contributes to the active energy accumulation—see the
Positive-Only Accumulation Mode section.
The output of the multiplier is divided by WDIV. If the value in
the WDIV register is equal to 0, then the internal active energy
register is divided by 1. WDIV is an 8-bit unsigned register.
After dividing by WDIV, the active energy is accumulated in a
49-bit internal energy accumulation register. The upper 24 bits
of this register are accessible through a read to the active energy
register (AENERGY[23:0]). A read to the RAENERGY register
returns the content of the AENERGY register and the upper 24
bits of the internal register are cleared. As shown in Figure 65, the
active power signal is accumulated in an internal 49-bit signed
register. The active power signal can be read from the waveform
register by setting MODE[14:13] = 0,0 and setting the WSMP
bit (Bit 3) in the interrupt enable register to 1. Like the Channel
APOS [15:0]
6
2
+
+
FORWAVEF0RM
-8
WGAIN[11:0]
24
32
0x19999
FOR WAVEFORM
ACCUMULATIOIN
0xCCCCD
SAMPLIN G
02875-0-064
1 and Channel 2 waveform sampling modes, the waveform date
is available at sample rates of 27.9 kSPS, 14 kSPS, 7 kSPS, or
3.5 kSPS—see Figure 52.
Figure 66 shows this energy accumulation for full-scale signals
(sinusoidal) on the analog inputs. The three curves displayed
illustrate the minimum period of time it takes the energy register
to roll over when the active power gain register contents are
0x7FF, 0x000, and 0x800. The watt gain register is used to carry
out power calibration in the ADE7753. As shown, the fastest
integration time occurs when the watt gain register is set to
maximum full scale, i.e., 0x7FF.
AENERGY [23:0]
0x7F,FFFF
0x3F,FFFF
0x00,0000
0x40,0000
0x80,0000
Figure 66. Energy Register Rollover Time for Full-Scale Power
6.248
(Minimum and Maximum Power Gain)
12.5
02875-0-065
WGAIN = 0x7FF
WGAIN = 0x000
WGAIN = 0x800
TIME (minutes)
Note that the energy register contents rolls over to full-scale
negative (0x800000) and continues to increase in value when
the power or energy flow is positive—see Figure 66. Conversely,
if the power is negative, the energy register underflows to fullscale positive (0x7FFFFF) and continues to decrease in value.
By using the interrupt enable register, the ADE7753 can be
IRQ
configured to issue an interrupt (
) when the active energy
register is half-full (positive or negative) or when an overflow or
underflow occurs.
Rev. A | Page 29 of 60
Page 30
ADE7753
Integration Time under Steady Load
As mentioned in the last section, the discrete time sample
period (T) for the accumulation register is 1.1 µs (4/CLKIN).
With full-scale sinusoidal signals on the analog inputs and the
WGAIN register set to 0x000, the average word value from each
LPF2 is 0xCCCCD—see Figure 61. The maximum positive
48
value that can be stored in the internal 49-bit register is 2
or
0xFFFF,FFFF,FFFF before it overflows. The integration time
under these conditions with WDIV = 0 is calculated as follows:
FFFFFFFF,xFFFF,0
Tim e =
xCCCCD0
× 1.12 µs = 375.8 s = 6.26 min (15)
When WDIV is set to a value different from 0, the integration
time varies, as shown in Equation 16.
WDIVTimeTime
WDIV×==0
(16)
POWER OFFSET CALIBRATION
The ADE7753 also incorporates an active power offset register
(APOS[15:0]). This is a signed twos complement 16-bit register
that can be used to remove offsets in the active power
calculation—see Figure 65. An offset could exist in the power
calculation due to crosstalk between channels on the PCB or in
the IC itself. The offset calibration allows the contents of the
active power register to be maintained at 0 when no power is
being consumed.
CFNUM[11:0]
110
DFC
480
AENERGY[48:0]
110
Figure 67. ADE7753 Energy-to-Frequency Conversion
%
CFDEN[11:0]
CF
02875-0-066
A digital-to-frequency converter (DFC) is used to generate the
CF pulsed output. The DFC generates a pulse each time 1 LSB
in the active energy register is accumulated. An output pulse is
generated when (CFDEN + 1)/(CFNUM + 1) number of pulses
are generated at the DFC output. Under steady load conditions,
the output frequency is proportional to the active power.
The maximum output frequency, with ac input signals at full
scale and CFNUM = 0x00 and CFDEN = 0x00, is approximately
23 kHz.
The ADE7753 incorporates two registers, CFNUM[11:0] and
CFDEN[11:0], to set the CF frequency. These are unsigned
12-bit registers, which can be used to adjust the CF frequency to
a wide range of values. These frequency-scaling registers are
12
12-bit registers, which can scale the output frequency by 1/2
12
1 with a step of 1/2
.
to
The 256 LSBs (APOS = 0x0100) written to the active power
offset register are equivalent to 1 LSB in the waveform sample
register. Assuming the average value, output from LPF2 is
0xCCCCD (838,861d) when inputs on Channels 1 and 2 are
both at full scale. At −60 dB down on Channel 1 (1/1000 of the
Channel 1 full-scale input), the average word value output from
LPF2 is 838.861 (838,861/1,000). One LSB in the LPF2 output
has a measurement error of 1/838.861 × 100% = 0.119% of the
average value. The active power offset register has a resolution
equal to 1/256 LSB of the waveform register, therefore the power
offset correction resolution is 0.00047%/LSB (0.119%/256) at
–60 dB.
ENERGY-TO-FREQUENCY CONVERSION
ADE7753 also provides energy-to-frequency conversion for
calibration purposes. After initial calibration at manufacturing,
the manufacturer or end customer often verify the energy meter
calibration. One convenient way to verify the meter calibration
is for the manufacturer to provide an output frequency, which is
proportional to the energy or active power under steady load
conditions. This output frequency can provide a simple, singlewire, optically isolated interface to external calibration equipment.
Figure 67 illustrates the energy-to-frequency conversion in the
ADE7753.
If the value 0 is written to any of these registers, the value 1
would be applied to the register. The ratio (CFNUM + 1)/
(CFDEN + 1) should be smaller than 1 to ensure proper
operation. If the ratio of the registers (CFNUM + 1)/(CFDEN + 1)
is greater than 1, the register values would be adjusted to a ratio
(CFNUM + 1)/(CFDEN + 1) of 1. For example, if the output
frequency is 1.562 kHz while the contents of CFDEN are 0
(0x000), then the output frequency can be set to 6.1 Hz by
writing 0xFF to the CFDEN register.
The output frequency has a slight ripple at a frequency equal to
twice the line frequency. This is due to imperfect filtering of the
instantaneous power signal to generate the active power signal—
see the Active Power Calculation section. Equation 9 from the
Active Power Calculation section gives an expression for the
instantaneous power signal. This is filtered by LPF2, which has a
magnitude response given by Equation 17.
1
fH+=
)(
1
(17)
2
f
2
9.8
Rev. A | Page 30 of 60
Page 31
ADE7753
The active power signal (output of LPF2) can be rewritten as
⎤
⎥
⎥
VI
2f
⎛
⎜
⎝
× cos(4πfLt) (18)
⎥
2
⎥
⎞
L
⎥
⎟
9.8
⎠
⎥
⎦
p(t) = VI −
where f
⎡
⎢
⎢
⎢
⎢
1
+
⎢
⎢
⎣
is the line frequency, for example, 60 Hz.
L
From Equation 13,
⎤
⎥
⎥
× sin(4πfLt) (19)
⎥
2
⎥
2f
⎞
L
⎥
⎟
9.8
⎠
⎥
⎦
E(t) = VIt −
⎡
⎢
⎢
⎢
⎢
⎢
⎢
⎣
VI
⎛
f
14
+π
⎜
L
⎝
From Equation 19 it can be seen that there is a small ripple in
the energy calculation due to a sin(2 ωt) component. This is
shown graphically in Figure 68. The active energy calculation is
shown by the dashed straight line and is equal to V × I × t. The
sinusoidal ripple in the active energy calculation is also shown.
WGAIN[11:0]
OUTPUT
FROM
LPF2
%
+
Since the average value of a sinusoid is 0, this ripple does not
contribute to the energy calculation over time. However, the
ripple can be observed in the frequency output, especially at
higher output frequencies. The ripple gets larger as a percentage
of the frequency at larger loads and higher output frequencies.
The reason is simply that at higher output frequencies the
integration or averaging time in the energy-to-frequency
conversion process is shorter. As a consequence, some of the
sinusoidal ripple is observable in the frequency output. Choosing
a lower output frequency at CF for calibration can significantly
reduce t he ripple. Als o, averaging the output fre quency by using
a longer gate time for the counter achieves the same results.
E(t)
Figure 68. Output Frequency Ripple
480
+
–
4×π×f
Vlt
VI
(1+2×fL/8.9Hz)
L
t
sin(4×π×f
02875-0-067
×t)
L
WDIV[7:0]APOS[15:0]
ACCUMULATE ACTIVE
FROM
CHANNEL 2
ADC
LPF1
230
ZERO CROSS
DETECTION
Figure 69. Energy Calculation Line Cycle Energy Accumulation Mode
CALIBRATION
CONTROL
LINECYC [15:0]
LAENERGY [23:0]
ENERGY IN INTERNAL
REGISTER AND UPDATE
THE LAENERGY REGISTER
AT THE END OF LINECYC
LINE CYCLES
02875-0-068
Rev. A | Page 31 of 60
Page 32
ADE7753
A
Y
LINE CYCLE ENERGY ACCUMULATION MODE
In line cycle energy accumulation mode, the energy accumulation of the ADE7753 can be synchronized to the Channel 2 zero
crossing so that active energy can be accumulated over an
integral number of half line cycles. The advantage of summing
the active energy over an integer number of line cycles is that
the sinusoidal component in the active energy is reduced to 0.
This eliminates any ripple in the energy calculation. Energy is
calculated more accurately and in a shorter time because the
integration period can be shortened. By using the line cycle
energy accumulation mode, the energy calibration can be
greatly simplified, and the time required to calibrate the meter
can be significantly reduced. The ADE7753 is placed in line
cycle energy accumulation mode by setting Bit 7 (CYCMODE)
in the mode register. In line cycle energy accumulation mode,
the ADE7753 accumulates the active power signal in the
LAENERGY register (Address 0x04) for an integral number of
line cycles, as shown in Figure 69. The number of half line
cycles is specified in the LINECYC register (Address 0x1C). The
ADE7753 can accumulate active power for up to 65,535 half
line cycles. Because the active power is integrated on an integral
number of line cycles, at the end of a line cycle energy accumulation cycle the CYCEND flag in the interrupt status register is
set (Bit 2). If the CYCEND enable bit in the interrupt enable
IRQ
register is enabled, the
IRQ
line can also be used to signal the completion of the line
cycle energy accumulation. Another calibration cycle can start
as long as the CYCMODE bit in the mode register is set.
output also goes active low. Thus the
Note that in this mode, the 16-bit LINECYC register can hold a
maximum value of 65,535. In other words, the line energy
accumulation mode can be used to accumulate active energy for
a maximum duration over 65,535 half line cycles. At 60 Hz line
frequency, it translates to a total duration of 65,535/120 Hz =
546 seconds.
POSITIVE-ONLY ACCUMULATION MODE
In positive-only accumulation mode, the energy accumulation
is done only for positive power, ignoring any occurrence of
negative power above or below the no-load threshold, as shown
in Figure 70. The CF pulse also reflects this accumulation
method when in this mode. The ADE7753 is placed in positiveonly accumulation mode by setting the MSB of the mode
register (MODE[15]). The default setting for this mode is off.
Transitions in the direction of power flow, going from negative
IRQ
to positive or positive to negative, set the
if the interrupt enable register is enabled. The interrupt status
registers, PPOS and PNEG, show which transition has
occurred—see the ADE7753 register descriptions in Table 10.
CTIVE ENERG
pin to active low
From Equations 13 and 18,
⎧
⎪
⎪
⎪
dtVI
E(t) =
−
⎨
0
⎪
1
+
⎪
⎪
⎩
where:
VI
⎛
⎜
⎝
⎫
⎪
nTnT
⎪
⎪
cos
(2πft)dt (20)
⎬
2
∫∫
⎪
f
⎞
0
⎟
⎪
9.8
⎪
⎠
⎭
NO-LOAD
THRESHOLD
ACTIVE POWER
NO-LOAD
THRESHOLD
IRQ
PPOSPNEGPNEG
INTERRUPT STATUS REGISTERS
n is an integer.
T is the line cycle period.
Since the sinusoidal component is integrated over an integer
number of line cycles, its value is always 0. Therefore,
nT
VIdt
E =
+ 0 (21)
∫
0
E(t) = VInT (22)
Figure 70. Energy Accumulation in Positive-Only Accumulation Mode
NO-LOAD THRESHOLD
The ADE7753 includes a no-load threshold feature on the active
energy that eliminates any creep effects in the meter. The
ADE7753 accomplishes this by not accumulating energy if the
multiplier output is below the no-load threshold. This threshold
is 0.001% of the full-scale output frequency of the multiplier.
Compare this value to the IEC1036 specification, which states
that the meter must start up with a load equal to or less than
0.4% Ib. This standard translates to .0167% of the full-scale
output frequency of the multiplier.
PNEGPPOSPPOS
02875-0-069
Rev. A | Page 32 of 60
Page 33
ADE7753
REACTIVE POWER CALCULATION
Reactive power is defined as the product of the voltage and
current waveforms when one of these signals is phase-shifted by
90°. The resulting waveform is called the instantaneous reactive
power signal. Equation 25 gives an expression for the instantaneous reactive power signal in an ac system when the phase of
the current channel is shifted by +90°.
The average reactive power over an integral number of lines (n)
is given in Equation 26.
nT
RP
nT
1
∫
0
==
VIdttRp
)sin()(
θ
(26)
where:
v(t) =
i(t) =
′
sin2)(
)sin(2θ+ωtV (23)
)sin(2tIω
π
⎞
⎛
tIti (24)
+ω=
⎟
⎜
2
⎠
⎝
where:
θ is the phase difference between the voltage and current
channel.
V is the rms voltage.
I is the rms current.
Rp(t) = v(t) × i’(t) (25)
90 DEGREE
PHASE SHIFT
I
MULTIPLIER
V
)2(θ+ωt
INSTANTANEOUS REACTIVE
π
2
ZERO-CROSSING
POWER SIGNAL (Rp(t))
DETECTION
LPF2
Rp(t) = VI sin (
CHANNEL 2
θ) + VI sin
FROM
ADC
LPF1
+
+
CALIBRATION
CONTROL
T is the line cycle period.
RP is referred to as the reactive power.
Note that the reactive power is equal to the dc component of the
instantaneous reactive power signal Rp(t) in Equation 25. This
is the relationship used to calculate reactive power in the
ADE7753. The instantaneous reactive power signal Rp(t) is
generated by multiplying Channel 1 and Channel 2. In this case,
the phase of Channel 1 is shifted by +90°. The dc component of
the instantaneous reactive power signal is then extracted by a
low-pass filter in order to obtain the reactive power information. Figure 71 shows the signal processing in the reactive power
calculation in the ADE7753.
490
ACCUMULATE REACTIVE
ENERGY IN INTERNAL
230
LVARENERGY [23:0]
REGISTER AND UPDATE
THE LVARENERGY REGISTER
AT THE END OF LINECYC HALF
LINE CYCLES
LINECYC [15:0]
Figure 71. Reactive Power Signal Processing
Rev. A | Page 33 of 60
02875-0-070
Page 34
ADE7753
ω
×
=
The features of the line reactive energy accumulation are the
same as the line active energy accumulation. The number of
half line cycles is specified in the LINECYC register. LINECYC
is an unsigned 16-bit register. The ADE7753 can accumulate
reactive power for up to 65535 combined half cycles. At the end
of an energy calibration cycle, the CYCEND flag in the interrupt
status register is set. If the CYCEND mask bit in the interrupt
IRQ
mask register is enabled, the
IRQ
Thus the
line can also be used to signal the end of a calibration. The ADE7753 accumulates the reactive power signal in
the LVARENERGY register for an integer number of half cycles,
as shown in Figure 71.
SIGN OF REACTIVE POWER CALCULATION
Note that the average reactive power is a signed calculation. The
phase shift filter has –90° phase shift when the integrator is
enabled, and +90° phase shift when the integrator is disabled.
Table 7 summarizes the relationship between the phase difference between the voltage and the current and the sign of the
resulting VAR calculation.
Table 7. Sign of Reactive Power Calculation
Angle Integrator Sign
Between 0° to 90°
Between –90° to 0°
Between 0° to 90°
Between –90° to 0°
APPARENT POWER CALCULATION
The apparent power is defined as the maximum power that can
be delivered to a load. V
current delivered to the load; the apparent power (AP) is defined
× I
as V
rms
. The angle θ between the active power and the
rms
apparent power generally represents the phase shift due to nonresistive loads. For single-phase applications, θ represents the
angle between the voltage and the current signals—see Figure 72.
Equation 28 gives an expression of the instantaneous power
signal in an ac system with a phase shift.
REACTIVE
POWER
rms
Figure 72. Power Triangle
output also goes active low.
Off Positive
Off Negative
On Positive
On Negative
and I
are the effective voltage and
rms
APPARENT
POWER
θ
ACTIVE
POWER
02875-0-071
()2sin( )
vtVt
=
rms
i(t) =
rms
p(t) =
The apparent power is defined as V
)sin(2θ+ωtI
(27)
)()()(titvtp
(28)
rmsrmsrmsrms
× I
rmsrms
)2cos()cos(θ+ω−θtIVIV
. This expression is
independent from the phase angle between the current and the
voltage.
Figure 73 illustrates the signal processing in each phase for the
calculation of the apparent power in the ADE7753.
I
rms
CURRENT RMS SIGNAL – i(t)
0x1C82B3
0x00
V
rms
VOLTAGE RMSSIGNAL– v(t)
0x17D338
0x00
Figure 73. Apparent Power Signal Processing
MULTIPLIER
VAGAIN
APPARENT POWER
SIGNAL(P)
0xAD055
02875-0-072
The gain of the apparent energy can be adjusted by using the
multiplier and VAGAIN register (VAGAIN[11:0]). The gain is
adjusted by writing a twos complement, 12-bit word to the
VAGAIN register. Equation 29 shows how the gain adjustment
is related to the contents of the VAGAIN register.
⎛
⎜
⎜
⎝
PowerApparentINOutputVAGA
⎧
1
⎨
⎩
VAGAIN
+×=
2
⎞
⎫
⎟
(29)
⎬
⎟
12
⎭
⎠
For example, when 0x7FF is written to the VAGAIN register, the
power output is scaled up by 50%. 0x7FF = 2047d, 2047/2
12
=
0.5. Similarly, 0x800 = –2047d (signed twos complement) and
power output is scaled by –50%. Each LSB represents 0.0244%
of the power output. The apparent power is calculated with the
current and voltage rms values obtained in the rms blocks of
the ADE7753. Figure 74 shows the maximum code (hexadecimal) output range of the apparent power signal. Note that the
output range changes depending on the contents of the apparent
power gain registers. The minimum output range is given when
the apparent power gain register content is equal to 0x800 and
the maximum range is given by writing 0x7FF to the apparent
power gain register. This can be used to calibrate the apparent
power (or energy) calculation in the ADE7753.
Rev. A | Page 34 of 60
Page 35
ADE7753
0
APPARENT POWER 100% FS
0x103880
0xAD055
0x5682B
0x00000
Figure 74. Apparent Power Calculation Output Range
APPARENT POWER 150% FS
0x0000x7FF0x800
{VAGAIN[11:0]}
APPARENT POWER
CALIBRATION RANGE
VOLTAGE AND CURRENT
CHANNEL INPUTS: 0.5V/GAIN
APPARENT POWER 50% FS
02875-0-073
Apparent Power Offset Calibration
Each rms measurement includes an offset compensation
register to calibrate and eliminate the dc component in the rms
value—see Channel 1 RMS Calculation and Channel 2 RMS
Calculation sections. The Channel 1 and Channel 2 rms values
are then multiplied together in the apparent power signal
processing. Since no additional offsets are created in the
multiplication of the rms values, there is no specific offset
compensation in the apparent power signal processing. The
offset compensation of the apparent power measurement is
done by calibrating each individual rms measurement.
APPARENT ENERGY CALCULATION
The apparent energy is given as the integral of the apparent
power.
The 49 bits of the internal register are divided by VADIV. If the
value in the VADIV register is 0, then the internal active energy
register is divided by 1. VADIV is an 8-bit unsigned register. The
upper 24 bits are then written in the 24-bit apparent energy
register (VAENERGY[23:0]). RVAENERGY register (24 bits
long) is provided to read the apparent energy. This register is
reset to 0 after a read operation.
Figure 76 shows this apparent energy accumulation for full-scale
signals (sinusoidal) on the analog inputs. The three curves
displayed illustrate the minimum time it takes the energy register
to roll over when the VAGAIN registers content is equal to 0x7FF,
0x000, and 0x800. The VAGAIN register is used to carry out an
apparent power calibration in the ADE7753. As shown, the fastest
integration time occurs when the VAGAIN register is set to
maximum full scale, i.e., 0x7FF.
VAENERGY [23:0]
230
480
%
APPARENT POWER
VADIV
480
+
+
=dttPowerApparentEnergyApparent)(
∫
(30)
The ADE7753 achieves the integration of the apparent power
signal by continuously accumulating the apparent power signal
in an internal 48-bit register. The apparent energy register
(VAENERGY[23:0]) represents the upper 24 bits of this internal
register. This discrete time accumulation or summation is
equivalent to integration in continuous time. Equation 31
expresses the relationship
∞
⎧
⎪
⎨
∑
T
0
⎪
n
=→0
⎩
×=
)(
⎫
⎪
(31)
TnTPowerApparentLimEnergyApparent
⎬
⎪
⎭
where:
n is the discrete time sample number.
T is the sample period.
The discrete time sample period (T) for the accumulation
register in the ADE7753 is 1.1 µs (4/CLKIN).
Figure 75 shows this discrete time integration or accumulation.
The apparent power signal is continuously added to the internal
register. This addition is a signed addition even if the apparent
energy remains theoretically always positive.
ACTIVEPOWER
SIGNAL= P
T
TIME (nT)
Figure 75. ADE7753 Apparent Energy Calculation
VAENERGY[23:0]
xFF,FFFF
0x80,0000
0x40,0000
0x20,0000
0x00,0000
Figure 76. Energy Register Rollover Time for Full-Scale Power
6.2612.5218.7825.04
(Maximum and Minimum Power Gain)
APPARENTPOWERARE
ACCUMULATED(INTEGRATED) IN
THEAPPARENTENERGY REGISTER
02875-0-074
VAGAIN = 0x7FF
VAGAIN = 0x000
VAGAIN = 0x800
TIME (minutes)
02875-0-075
Rev. A | Page 35 of 60
Page 36
ADE7753
Note that the apparent energy register is unsigned—see Figure 76.
By using the interrupt enable register, the ADE7753 can be configured to issue an interrupt (
register is half full or when an overflow occurs. The half full
interrupt for the unsigned apparent energy register is based on
24 bits as opposed to 23 bits for the signed active energy register.
Integration Times under Steady Load
As mentioned in the last section, the discrete time sample
period (T) for the accumulation register is 1.1 µs (4/CLKIN).
With full-scale sinusoidal signals on the analog inputs and the
VAGAIN register set to 0x000, the average word value from
apparent power stage is 0xAD055—see the Apparent Power
Calculation section. The maximum value that can be stored in
the apparent energy register before it overflows is 2
0xFF,FFFF. The average word value is added to the internal
register, which can store 2
overflows. Therefore, the integration time under these conditions
with VADIV = 0 is calculated as follows:
Time =
When VADIV is set to a value different from 0, the integration
time varies, as shown in Equation 33.
Time = Ti me
WDIV = 0
IRQ
) when the apparent energy
24
or
48
or 0xFFFF,FFFF,FFFF before it
FFFFFFFF,xFFFF,0
055xD0
× 1.2 µs = 888 s = 12.52 min (32)
× VA DI V (33)
LINE APPARENT ENERGY ACCUMULATION
The ADE7753 is designed with a special apparent energy
accumulation mode, which simplifies the calibration process.
By using the on-chip zero-crossing detection, the ADE7753
accumulates the apparent power signal in the LVAENERGY
register for an integral number of half cycles, as shown in
Figure 77. The line apparent energy accumulation mode is
always active.
The number of half line cycles is specified in the LINCYC
register, which is an unsigned 16-bit register. The ADE7753 can
accumulate apparent power for up to 65535 combined half
cycles. Because the apparent power is integrated on the same
integral number of line cycles as the line active energy register,
these two values can be compared easily. The active energy and
the apparent energy are calculated more accurately because of
this precise timing control and provide all the information
needed for reactive power and power factor calculation. At the
end of an energy calibration cycle, the CYCEND flag in the
interrupt status register is set. If the CYCEND mask bit in the
IRQ
interrupt mask register is enabled, the
IRQ
active low. Thus the
line can also be used to signal the end
of a calibration.
The line apparent energy accumulation uses the same signal
path as the apparent energy accumulation. The LSB size of these
two registers is equivalent.
output also goes
480
230
LVAENERGY [23:0]
LVAENERGY REGISTER IS
UPDATED EVERY LINECYC
ZERO CROSSINGS WITH THE
TOTAL APPARENT ENERGY
DURING THAT DURATION
02875-0-076
FROM
CHANNEL 2
ADC
LPF1
APPARENT
POWER
ZERO-CROSSING
DETECTION
Figure 77. ADE7753 Apparent Energy Calibration
%
VADIV[7:0]
CALIBRATION
LINECYC [15:0]
+
CONTROL
+
Rev. A | Page 36 of 60
Page 37
ADE7753
ENERGIES SCALING
The ADE7753 provides measurements of active, reactive, and
apparent energies. These measurements do not have the same
scaling and thus cannot be compared directly to each other.
When using a reference meter, the ADE7753 calibration output
frequency, CF, is adjusted to match the frequency output of the
reference meter. A pulse output is only provided for the active
energy measurement in the ADE7753. If it is desired to use a
reference meter for calibrating the VA and VAR, then additional
code would have to be written in a microprocessor to produce a
pulsed output for these quantities. Otherwise, VA and VAR
calibration require an accurate source.
The ADE7753 provides a line cycle accumulation mode for
calibration using an accurate source. In this method, the active
energy accumulation rate is adjusted to produce a desired CF
frequency. The benefit of using this mode is that the effect of
the ripple noise in the active energy is eliminated. Up to 65535
half line cycles can be accumulated, thus providing a stable
energy value to average. The accumulation time is calculated
from the line cycle period, measured by the ADE7753 in the
PERIOD register, and the number of half line cycles in the
accumulation, fixed by the LINECYC register.
Current and voltage rms offset calibration removes any apparent
energy offset. A gain calibration is also provided for apparent
energy. Figure 79 shows an optimized calibration flow for active
energy, rms, and apparent energy.
CALIBRATING AN ENERGY METER BASED ON THE
ADE7753
The ADE7753 provides gain and offset compensation for active
and apparent energy calibration. Its phase compensation corrects
phase error in active, apparent and reactive energy. If a shunt is
used, offset and phase calibration may not be required. A
reference meter or an accurate source can be used to calibrate
the ADE7753.
WATT/VA GAIN CALIBRATION
RMS CALIBRATION
Figure 79. Apparent and Active Energy Calibration
Active and apparent energy gain calibrations can take place
concurrently, with a read of the accumulated apparent energy
register following that of the accumulated active energy register.
Figure 78 shows the calibration flow for the active energy
portion of the ADE7753.
WATT GAIN CALIBRATIONWATT OFFSET CALIBRATIONPHASE CALIBRATION
Figure 78. Active Energy Calibration
The ADE7753 does not provide means to calibrate reactive
energy gain and offset. The reactive energy portion of the
ADE7753 can be calibrated externally, through a MCU.
WATT OFFSET CALIBRATION
PHASE CALIBRATION
02875-A-002
02875-A-005
Rev. A | Page 37 of 60
Page 38
ADE7753
Watt Gain
The first step of calibrating the gain is to define the line voltage,
base current and the maximum current for the meter. A meter
constant needs to be determined for CF, such as 3200 imp/kWh
or 3.2 imp/Wh. Note that the line voltage and the maximum
current scale to half of their respective analog input ranges in
this example.
The expected CF in Hz is
(Hz) =
CF
expected
(W)(imp/Wh)ϕ×× LoadantMeterConst
s/h3600
where
is the angle between I and V, and cos is the power
ϕ
factor.
The ratio of active energy LSBs per CF pulse is adjusted using
the CFNUM, CFDEN, and WDIV registers.
expected
onTimeAccumulati
WDIV
(s)+
LAENERGY
=
CF
The relationship between watt-hours accumulated and the
quantity read from AENERGY can be determined from the
amount of active energy accumulated over time with a given
load:
Wh
LSB
=
×
s/3600
×
where Accumulation Time can be determined from the value in
the line period and the number of half line cycles fixed in the
LINECYC register.
Accumulation time(s) =
IB
The line period can be determined from the PERIOD register:
Line Period(s) = PERIOD ×
8
CLKIN
The AENERGY Wh/LSB ratio can also be expressed in terms of
the meter constant:
)1(
+
)1(
+
(imp/Wh)
antMeterConst
WDIV
×
Wh
LSB
=
CFNUM
CFDEN
In a meter design, WDIV, CFNUM, and CFDEN should be kept
constant across all meters to ensure that the Wh/LSB constant is
maintained. Leaving WDIV at its default value of 0 ensures
maximum resolution. The WDIV register is not included in the
CF signal chain so it does not affect the frequency pulse output.
)cos(
(34)
)(ϕ
)1(
+
(35)
)1(
(36)
(s)PeriodLineLINECYC
(37)
TimeonAccumulatiLoad
hLAENERGY
×
××
2
CFNUM
CFDEN
(s)(W)
(38)
(39)
The WGAIN register is used to finely calibrate each meter. Calibrating the WGAIN register changes both CF and AENERGY for
a given load condition.
AENERGY
CF
expected
= AENERGY ×(40)
expected
(Hz) = CF × (41)
nominal
CFNUM
CFDEN
nominal
⎛
1
+
⎜
⎜
⎝
)1(WGAIN
+
)1(
+
WGAIN
12
2
⎛
1
+×
⎜
⎜
⎝
⎞
⎟
⎟
⎠
⎞
⎟
⎟
12
2
⎠
When calibrating with a reference meter, WGAIN is adjusted
until CF matches the reference meter pulse output. If an accurate
source is used to calibrate, WGAIN is modified until the active
energy accumulation rate yields the expected CF pulse rate.
The steps of designing and calibrating the active energy portion
of a meter with either a reference meter or an accurate source
are outlined in the following examples. The specifications for
this example are
Meter Constant: MeterConstant(imp/Wh) = 3.2
Base Current: I
Maximum Current: I
Line Voltage: V
Line Frequency: f
= 10 A
b
= 60 A
MAX
= 220 V
nominal
= 50 Hz
l
The first step in calibration with either a reference meter or an
accurate source is to calculate the CF denominator, CFDEN.
This is done by comparing the expected CF pulse output to the
nominal CF output with the default CFDEN = 0x3F and
CFNUM = 0x3F and when the base current is applied.
The expected CF output for this meter with the base current
applied is 1.9556 Hz using Equation 34.
IB(expected)
(Hz) =
V220A10imp/Wh200.3
××
s/h3600
can be measured from a reference meter
expected
=ϕ×
Hz9556.1)cos(
CF
Alternatively, CF
pulse output if available.
CF
(Hz) = CF(42)
expected
ref
The maximum CF frequency measured without any frequency
division and with ac inputs at full scale is 23 kHz. For this
example, the nominal CF with the test current, I
, applied is
b
958 Hz. In this example the line voltage and maximum current
scale half of their respective analog input ranges. The line
voltage and maximum current should not be fixed at the
maximum analog inputs to account for occurrences such as
spikes on the line.
I
1
(Hz) = (43)
CF
nominal
1
kHz23
×××
2
2
I
MAX
Rev. A | Page 38 of 60
CF
(Hz) =
IB(nominal)
kHz23=×××
2
2
10
1
1
60
Hz958
Page 39
ADE7753
The nominal CF on a sample set of meters should be measured
using the default CFDEN, CFNUM, and WDIV to ensure that
the best CFDEN is chosen for the design.
With the CFNUM register set to 0, CFDEN is calculated to be
489 for the example meter:
CFDEN =
CFDEN =
INT
INT
⎛
CF
⎜
⎜
CF
expectedIB
⎝
958
⎛
⎜
9556.1
⎝
⎞
)(
nominalIB
⎟
1
−
(44)
⎟
)(
⎠
⎞
⎟
489)1490(1
=−=−
⎠
This value for CFDEN should be loaded into each meter before
calibration. The WGAIN and WDIV registers can then be used
to finely calibrate the CF output. The following sections explain
how to calibrate a meter based on ADE7753 when using a
reference meter or an accurate source.
Calibrating Watt Gain Using a Reference Meter Example
The CFDEN and CFNUM values for the design should be
written to their respective registers before beginning the
calibration steps shown in Figure 80. When using a reference
meter, the %ERROR in CF is measured by comparing the CF
output of the ADE7753 meter with the pulse output of the
reference meter with the same test conditions applied to both
meters. Equation 45 defines the percent error with respect to
the pulse outputs of both meters (using the base current, I
):
b
For this example:
Meter Constant: MeterConstant(imp/Wh) = 3.2
CF Numerator: CFNUM = 0
CF Denominator: CFDEN = 489
% Error measured at Base Current:
%ERROR
CF(IB)
= -3.07%
One LSB change in WGAIN changes the active energy registers
and CF by 0.0244%. WGAIN is a signed twos complement
register and can correct for up to a 50% error. Assuming a
−3.07% error, WGAIN is 126:
WGAIN = INT
WGAIN = INT
⎛
⎜
−
⎜
⎝
−
⎛
⎜
⎝
%07.3
−
%0244.0
⎞
)(IBCF
⎟
(46)
⎟
%0244.0
⎠
⎞
126
=
⎟
⎠
%
ERROR
When CF is calibrated, the AENERGY register has the same
Wh/LSB constant from meter to meter if the meter constant,
WDIV, and the CFNUM/CFDEN ratio remain the same. The
−4
Wh/LSB ratio for this meter is 6.378 × 10
using Equation 39
with WDIV at the default value.
)1(
+
)1(
+
(imp/Wh)
antMeterConst
WDIV
×
Wh
LSB
=
CFNUM
CFDEN
−
%ERROR
Figure 80. Calibrating Watt Gain Using a Reference Meter
= (45)
CF(IB)
CALCULATE CFDEN VALUE FOR DESIGN
WRITE CFDEN VALUE TO CFDEN REGISTER
SET I
MEASURE THE % ERROR BETWEEN
REFERENCE METER OUTPUT
CALCULATE WGAIN. SEE EQUATION 46.
WRITE WGAIN VALUE TO THE WGAIN
CFCF
CF
ADDR. 0x15 = CFDEN
= Ib, V
TEST
THE CF OUTPUT AND THE
REGISTER: ADDR. 0x12
IBref
TEST
)(
IBrefIB
100
×
)(
= V
, PF = 1
NOM
02875-A-006
1
Wh
LSB
)1490(
=
+
imp/Wh200.3
1
=
2.3490
×
4
−
10378.6
×=
Calibrating Watt Gain Using an Accurate Source Example
The CFDEN value calculated using Equation 44 should be
written to the CFDEN register before beginning calibration and
zero should be written to the CFNUM register. First, the line
accumulation mode and the line accumulation interrupt should
be enabled. Next, the number of half line cycles for the energy
accumulation is written to the LINECYC register. This sets the
accumulation time. Reset the interrupt status register and wait for
the line cycle accumulation interrupt. The first line cycle
accumulation results may not have used the accumulation time
set by the LINECYC register and should be discarded. After
resetting the interrupt status register, the following line cycle
readings will be valid. When LINECYC half line cycles have
IRQ
elapsed, the
with the test current applied can be read. This LAENERGY
value is compared to the expected LAENERGY value to deter-
pin goes active low and the nominal LAENERGY
mine the WGAIN value. If apparent energy gain calibration is
performed at the same time, LVAENERGY can be read directly
after LAENERGY. Both registers should be read before the next
IRQ
interrupt is issued on the
pin. Refer to the Apparent Energy
Calculation section for more details. Figure 81 details the steps
that calibrate the watt gain using an accurate source.
Rev. A | Page 39 of 60
Page 40
ADE7753
CALCULATE CFDEN VALUE FOR DESIGN
WRITE CFDEN VALUE TO CFDEN REGISTER
SET HALF LINECYCLES FOR ACCUMULATION
ADDR. 0x15 = CFDEN
SET I
= Ib, V
TEST
IN LINECYC REGISTER ADDR. 0x1C
TEST
= V
NOM
, PF = 1
The nominal LAENERGY reading, LAENERGY
IB(nominal)
, is the
LAENERGY reading with the test current applied. The expected
LAENERGY reading is calculated from the following equation:
LAENERGY
⎛
⎜
⎜
INT
⎜
⎜
⎝
expectedIB
IB(expected)
CFNUM
CFDEN
=
⎞
×
)(
+
1
×
WDIV
+
1
⎟
(s)
TimeonAccumulatiCF
⎟
(48)
⎟
⎟
⎠
SET MODE FOR LINE CYCLE
ACCUMULATION ADDR. 0x09 = 0x0080
ENABLE LINE CYCLE ACCUMULATION
INTERRUPT ADDR. 0x0A = 0x04
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
INTERRUPT?
YES
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
INTERRUPT?
YES
READ LINE ACCUMULATION ENERGY
CALCULATE WGAIN. SEE EQUATION 47.
WRITE WGAIN VALUE TO THE WGAIN
Figure 81. Calibrating Watt Gain Using an Accurate Source
ADDR. 0x04
REGISTER: ADDR. 0x12
NO
NO
02875-A-007
Equation 47 describes the relationship between the expected
LAENERGY value and the LAENERGY measured in the test
condition:
WGAIN = INT
⎛
⎛
LAENERGY
⎜
⎜
⎜
⎜
LAENERGY
⎝
⎝
)(
expectedIB
nominalIB
−
)(
⎞
⎞
12
⎟
⎟
(47)
×
21
⎟
⎟
⎠
⎠
where CF
(Hz) is calculated from Equation 34, accumula-
IB(expected)
tion time is calculated from Equation 37, and the line period is
determined from the PERIOD register according to Equation 38.
For this example:
Meter Constant: MeterConstant(imp/Wh) = 3.2
Tes t Cu r re n t: I
Line Voltage: V
Line Frequency: f
Half Line Cycles: LINECYC
= 10 A
b
= 220 V
nominal
= 50 Hz
l
= 2000
IB
CF Numerator: CFNUM = 0
CF Denominator: CFDEN = 489
Energy Reading at Base Current:
LAENERGY
IB (nominal)
= 17174
Period Register Reading: PERIOD = 8959
Clock Frequency: CLKIN = 3.579545 MHz
is calculated to be 1.9556 Hz according to Equation 34.
CF
expected
LAENERGY
CF
IB(expected)
LAENERGY
⎛
⎜
⎜
INT
⎜
⎜
⎝
LAENERGY
⎛
⎜
⎜
INT
⎜
⎜
⎝
is calculated to be 19186 using Equation 48.
expected
(Hz) =
A10V220imp/Wh200.3
s/h3600
IB(expected)
IB(expected)
××
=
)(
CFNUM
CFDEN
=
)(cos(
ϕ×
= 1.9556 Hz
IBexpectedIB
+
1
×
WDIV
+
1
××××
1
1489
+
19186)4.19186(=INT
×××
CLKINPERIODLINECYCCF
/82/
⎞
⎟
6
)10579545.3/(889592/20009556.1
⎟
1
=
⎟
⎟
⎠
⎞
⎟
⎟
⎟
⎟
⎠
WGAIN is calculated to be 480 using Equation 47.
Note that WGAIN is a signed twos complement register.
Rev. A | Page 40 of 60
WGAIN = INT
⎛
⎛
⎜
⎜
⎜
⎝
⎝
19186
17174
⎞
⎞
12
−
⎟
48021
=
×
⎟
⎠
⎟
⎠
Page 41
ADE7753
With WDIV and CFNUM set to 0, LAENERGY can be
expressed as
LAENERGY =
The calculated Wh/LSB ratio for the active energy register, using
Equation 39 is 6.378 × 10
IB(expected)
)(
))1(/82/(
IBexpectedIB
−
4
:
+××××CFDENCLKINPERIODLINECYCCFINT
1
+
Wh
=
LSB
)1489(
imp/Wh200.3
4
−
10378.6
×=
For this example:
Meter Constant:
Minimum Current: I
Load at Minimum Current: W
CF Error at Minimum Current: %ERROR
Using Equation 49, APOS is calculated to be −522 for this example.
Watt Offset
Offset calibration allows outstanding performance over a wide
dynamic range, for example, 1000:1. To do this calibration two
measurements are needed at unity power factor, one at I
and
b
the other at the lowest current to be corrected. Either calibration
frequency or line cycle accumulation measurements can be
used to determine the energy offset. Gain calibration should be
performed prior to offset calibration.
Offset calibration is performed by determining the active
energy error rate. Once the active energy error rate has been
determined, the value to write to the APOS register to correct
the offset is calculated.
APOS = −
RateErrorAENERGY
CLKIN
(49)
35
2×
The AENERGY registers update at a rate of CLKIN/4. The twos
complement APOS register provides a fine adjustment to the
active power calculation. It represents a fixed amount of power
offset to be adjusted every CLKIN/4. The 8 LSBs of the APOS
register are fractional such that one LSB of APOS represents
1/256 of the least significant bit of the internal active energy
register. Therefore, one LSB of the APOS register represents 2
−
33
of the AENERGY[23:0] active energy register.
The steps involved in determining the active energy error rate
for both line accumulation and reference meter calibration
options are shown in the following sections.
Calibrating Watt Offset Using a Reference Meter Example
Figure 82 shows the steps involved in calibrating watt offset
with a reference meter.
SET I
= I
, V
= V
TEST
MIN
TEST
MEASURE THE % ERROR BETWEEN THE
CF OUTPUT AND THE REFERENCE METER
OUTPUT, AND THE LOAD IN WATTS
NOM
, PF = 1
CF Absolute Error = CF
IMIN(nominal)IMIN(expected)
− CF
(50)
CF Absolute Error =
(%ERROR
) × W
CF(IMIN)IMIN
× (51)
(imp/Wh)antMeterConst
3600
CF Absolute Error =
%3.1
⎛
⎞
⎜
⎟
100
⎝
⎠
200.3
6.9
3600
=××
Hz000110933.0
Then,
AENERGY Error Rate (LSB/s) =
CF Absolute Error ×
CFDEN
CFNUM
+
(52)
11+
AENERGY Error Rate (LSB/s) =
0.000110933 ×
=
1
490
05436.0
Using Equation 49, APOS is −522.
35
205436.0
APOS = −
×
×
522
−=
6
10579545.3
APOS can be represented as follows with CFNUM and WDIV
set at 0:
APOS =
(imp/Wh)
CLKIN
antMeterConst
3600
CFDEN
)(%×+×××
WERROR
−
IMINIMINCF35)(
2)1(
CALCULATE APOS. SEE EQUATION 49.
WRITE APOS VALUE TO THE APOS
REGISTER: ADDR. 0x11
Figure 82. Calibrating Watt Offset Using a Reference Meter
02875-A-008
Rev. A | Page 41 of 60
Page 42
ADE7753
Calibrating Watt Offset with an Accurate Source Example
Figure 83 is the flowchart for watt offset calibration with an
accurate source.
SET I
= I
, V
= V
TEST
MIN
TEST
NOM
, PF = 1
The LAENERGY
LAENERGY
⎛
I
MIN
⎜
INT
⎜
I
B
⎝
at I
expected
IMIN(expected)
LAENERGY
is 1370 using Equation 53.
MIN
=
LINECYCI
××
)(
expectedIB
LINECYC
MIN
IB
⎞
⎟
⎟
⎠
(53)
SET HALF LINE CYCLES FOR ACCUMULATION
IN LINECYC REGISTER ADDR. 0x1C
SET MODE FOR LINE CYCLE
ACCUMULATION ADDR. 0x09 = 0x0080
ENABLE LINE CYCLE ACCUMULATION
INTERRUPT ADDR. 0x0A = 0x04
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
INTERRUPT?
YES
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
INTERRUPT?
READ LINE ACCUMULATION ENERGY
CALCULATE APOS. SEE EQUATION 49.
YES
ADDR. 0x04
NO
NO
LAENERGY
04.0
⎛
INT
⎜
10
⎝
IMIN(expected)
19186
=
35700
2000
⎞
⎟
⎠
××INT
1370)80.1369(
==
where:
LAENERGY
is the expected LAENERGY reading at Ib
IB(expected)
from the watt gain calibration.
LINECYC
accumulated over when measuring at I
is the number of half line cycles that energy is
IMIN
.
MIN
More line cycles could be required at the minimum current to
minimize the effect of quantization error on the offset calibration.
For example, if a test current of 40 mA results in an active energy
accumulation of 113 after 2000 half line cycles, one LSB variation
in this reading represents an 0.8% error. This measurement does
not provide enough resolution to calibrate out a <1% offset
error. However, if the active energy is accumulated over 37,500
half line cycles, one LSB variation results in 0.05% error, reducing
the quantization error.
APOS is −672 using Equations 55 and 49.
LAENERGY Absolute Error =
LAENERGY
IMIN(nominal)
− LAENERGY
IMIN(expected)
WRITE APOS VALUE TO THE APOS
REGISTER: ADDR. 0x11
Figure 83. Calibrating Watt Offset with an Accurate Source
02875-A-009
For this example:
Meter Constant: MeterConstant(imp/Wh) = 3.2
Line Voltage: V
Line Frequency: f
= 220 V
nominal
= 50 Hz
l
CF Numerator: CFNUM = 0
CF Denominator: CFDEN = 489
Base Current: I
= 10 A
b
Half Line Cycles Used at Base Current: LINECYC
= 2000
(IB)
Period Register Reading: PERIOD = 8959
Clock Frequency: CLKIN = 3.579545 MHz
Expected LAENERGY Register Value at Base Current
(from the Watt Gain section):LAENERGY
Minimum Current: I
= 40 mA
MIN
IB(expected)
= 19186
Number of Half Line Cycles used at Minimum Current:
LINECYC
(IMIN)
= 35700
Active energy Reading at Minimum Current: LAENERGY
IMIN(nominal)
= 1395
LAENERGY Absolute Error = 1395 − 1370 = 25 (54)
AENERGY Error Rate (LSB/s) =
ErrorAbsoluteLAENERGY
LINECYC
CLKIN
PERIOD
××82/
(55)
AENERGY Error Rate (LSB/s) =
6
×
89598
10579545.3
×
CLKIN
2069948771.0
×
6
10579545.3
×
069948771.0
=
RateErrorAENERGY
35
672
−=
35
2×
25
2/35700
APOS = −
APOS = −
×
Rev. A | Page 42 of 60
Page 43
ADE7753
Phase Calibration Calibrating Phase Using a Reference Meter Example
The PHCAL register is provided to remove small phase errors.
The ADE7753 compensates for phase error by inserting a small
time delay or advance on the voltage channel input. Phase leads
up to 1.84° and phase lags up to 0.72° at 50 Hz can be corrected.
The error is determined by measuring the active energy at I
B
and two power factors, PF = 1 and PF =0.5 inductive.
A power factor of 0.5 inductive can be assumed if the pulse
output rate of the reference meter is half of its PF = 1 rate. Then
the %ERROR between CF and the pulse output of the reference
meter can be used to perform the preceding calculations.
SET I
TEST
= Ib, V
TEST
= V
NOM
, PF = 0.5
Some CTs may introduce large phase errors that are beyond the
range of the phase calibration register. In this case, coarse phase
compensation has to be done externally with an analog filter.
The phase error can be obtained from either CF or LAENERGY
measurements:
Error =
=
LAENERGY
LAENERGYLAENERGY−
expectedIB
expectedIBPFIB
2
)(
)(5.,
2
(56)
If watt gain and offset calibration have been performed, there
should be 0% error in CF at unity power factor and then:
Error = %ERROR
CF(IB,PF = .5)
/100 (57)
The phase error is
Phase Error (°) = −Arcsin
⎜
⎜
⎝
(58)
⎟
3
⎠
⎞
⎛
Error
⎟
The relationship between phase error and the PHCAL phase
correction register is
PHCAL=
INT
⎛
ErrorPhase0x0D (59)
⎜
⎝
()
PERIOD
⎞
+
⎟
°×°360
⎠
MEASURE THE % ERROR BETWEEN
THE CF OUTPUT AND THE
REFERENCE METER OUTPUT
CALCULATE PHCAL. SEE EQUATION 59.
WRITE PHCAL VALUE TO THE PHCAL
REGISTER: ADDR. 0x10
Figure 84. Calibrating Phase Using a Reference Meter
02875-A-010
For this example:
CF % Error at PF = .5 Inductive: %ERROR
CF(IB,PF = .5)
PERIOD Register Reading: PERIOD = 8959
Then PHCAL is 11 using Equations 57 through 59:
Error = 0.215% / 100 = 0.00215
Phase Error (°) = −Arcsin
⎛
PHCAL = INT
07.0
⎜
⎝
×°−
⎛
⎜
⎜
⎝
8959
360
⎞
00215.0
⎟
⎟
3
⎠
⎞
+0x0D = −2 + 13 = 11
⎟
°
⎠
°−=
07.0
PHCAL can be expressed as follows:
= 0.215%
The expression for PHCAL can be simplified using the
assumption that at small x:
Arcsin(x) ≈ x
The delay introduced in the voltage channel by PHCAL is
Delay = (PHCAL
− 0x0D) × 8/CLKIN (60)
The delay associated with the PHCAL register is a time delay if
(PHCAL − 0x0D) is positive but represents a time advance if
this quantity is negative. There is no time delay if PHCAL =
0x0D.
The phase correction is in the opposite direction of the phase
error.
Phase Correction (°) = −(PHCAL
− 0x0D) (61)
°×360
PERIOD
Rev. A | Page 43 of 60
PHCAL =
INT
⎛
⎜
⎜
⎝
−
Arcsin
⎞
⎛
⎜
⎜
⎝
PERIODError
⎟
×
⎟
3
⎠
⎞
⎟
+ 0x0D(62)
⎟
π
2
⎠
Note that PHCAL is a signed twos complement register.
Setting the PHCAL register to 11 provides a phase correction
of 0.08° to correct the phase lead:
°
360
8960
×−−
)(
PERIOD
°
360
°=
Phase Correction (°) =
Phase Correction (°) =
PHCAL
0x0D
0x0D
)11(
×−−08.0
Page 44
ADE7753
Calibrating Phase with an Accurate Source Example
With an accurate source, line cycle accumulation is a good
method of calibrating phase error. The value of LAENERGY
must be obtained at two power factors, PF = 1 and PF = 0.5
inductive.
SET I
TEST
= Ib, V
TEST
= V
NOM
, PF = 0.5
The error using Equation 56 is
191869613 −
Error =
Phase Er
19186
ror (°) = −Arcsin
2
=
2
0021.0
⎛
⎜
⎜
⎝
⎞
0021.0
⎟
⎟
3
⎠
°−=
07.0
SET HALF LINE CYCLES FOR ACCUMULATION
Figure 85. Calibrating Phase with an Accurate Source
For this example:
IN LINECYC REGISTER ADDR. 0x1C
SET MODE FOR LINE CYCLE
ACCUMULATION ADDR. 0x09 = 0x0080
ENABLE LINE CYCLE ACCUMULATION
INTERRUPT ADDR. 0x0A = 0x04
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
INTERRUPT?
YES
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
INTERRUPT?
YES
READ LINE ACCUMULATION ENERGY
CALCULATE PHCAL. SEE EQUATION 59.
WRITE PHCAL VALUE TO THE PHCAL
ADDR. 0x04
REGISTER: ADDR. 0x10
NO
NO
02875-A-011
Usinalculated to be 11g Equation 59, PHCAL is c.
8959
⎞⎛
×°−
07.0+−=+
⎜
⎝
Note a signed twos complement register.
that PHCAL is
360
0x0DPHCAL = INT
⎟
°
⎠
11132
=
The phase lead is corrected by 0.08° when the PHCAL register
is set to 11:
°
360
8960
×−−
)(
PERIOD
°
360
°=
Phase Correction (°) =
Phase Correction (°) =
PHCAL
0x0D
0x0D
)11(
×−−08.0
VRMS and IRMS Calibration
VRMted by squaring the input in a S and IRMS are calcula
digital multiplier.
222
2
The square of the rms value is extracted from v
(t) by a low-pass
filter. The square root of the output of this low-pass filter
ω×−=ω×ω=
)2cos()sin(V2)sin(V2)(tVVtttv
gives
(63)
the rms value. An offset correction is provided to cancel noise
and offset contributions from the input.
There is ripple noise from the 2ω term because the low-pass
filter does not completely attenuate the si
gnal. This noise can be
minimized by synchronizing the rms register readings with the
IRQ
zero crossing of the voltage signal. The
output can be
configured to indicate the zero crossing of the voltage signal.
This flowchart demonstrates how VRMS and IRMS readings ar
synchronized to the zero crossings of the voltage input.
SET INTERRUPT ENABLE FOR ZERO
CROSSING ADDR. 0x0A = 0x0010
e
Meter Constant: MeterConstant(imp/Wh) = 3.2
Line Voltage: V
Line Frequency: f
= 220 V
nominal
= 50 Hz
l
CF Numerator: CFNUM = 0
CF Denominator: CFDEN = 489
Base Current: I
= 10 A
b
Half Line Cycles Used at Base Current:
LINECYC
= 2000
IB
PERIOD Register: PERIOD = 8959
Expected Line Accumulation at Unity Power Factor (from Watt
Gain Section: LAENERGY = 19186
IB(expected)
Active Energy Reading at PF = .5 inductive:
LAENERGY
IB, PF = .5
= 9613
Rev. A | Page 44 of 60
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
INTERRUPT?
NO
YES
READ VRMS OR IRMS
ADDR. 0x17; 0x16
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. 0x0C
02875-A-003
Figure 86. Synchronizing VRMS and IRMS Readings with Zero Crossings
Page 45
ADE7753
Voltage rms compensation is done after the square root.
VRMS = VRMS0 + VRMSOS (64)
where:
VRMS0 is the rms measurement without offset correction.
VRMS is linear from full-scale to full-scale/20.
To calibrate the offset, two VRMS measurements are required,
for example, at V
nominal
and V
nominal
/10. V
is set at half of the
nominal
full-scale analog input range so the smallest linear VRMS
reading is at V
VRMSOS =
where VRMS
correction for input V
If thplement VRMSOS regist
e range of the 12-bit, twos comer is
not enou
gh, the voltage channel offset register, CH2OS, can be
/10.
nominal
and VRMS
12
and V , respectively.
12
VRMSVVRMSV
×−×
1221
VV
−
12
(65)
are rms register values without o
ffset
used to correct the VRMS offset.
Current rms compensation is performed before th
22
IRMS
= IRMS0
+ 32768 × IRMSOS (66
e square root:
where IRMS0 is the rms measurement without offset correction
The current rms calculation is linear from full-scale to full
-
scale/100.
To cffset, two IRMS measurem
alibrate this oents are required,
for example, at I
and I
b
MAX
/50. I
is set at half of the full-scale
MAX
analog input range so the smallest linear IRMS reading is at
/50.
I
MAX
IRMSOS =
where IRMS
1
32768
and IRMS
12
correction for input I
2
2
1
×
2
×−×
2
2
2
2
II
−
1
2
are rms register values without offset
and I , respectively.
12
2
IRMSIIRMSI
1
(67)
)
.
Apparent Energy
Apparent energy gain calibration is provided for both meter-tometer gain adjustment and for setting the VAh/LSB constant.
VAENERGY =
VAENERGY
initial
1VAGAIN
⎛
1
+××
VADIV
⎜
⎝
⎞
(68)
⎟
12
2
⎠
VA DI V is similar to the CFDEN for the watt hour calibration. It
should be the same across all meters and determines the VAh/LSB
constant. VA G AI N is used to calibrate individual meters.
Apparent energy gain calibration should be performed before
rms offset correction to make most efficient use of the current
test points. Apparent energy gain and watt gain compensation
require testing at I
while rms and watt offset correction require
b
a lower test current. Apparent energy gain calibration can be
done at the same time as the watt-hour gain calibration using
line cycle accumulation. In this case, LAENERGY and
LVA E N E RG Y , the line cycle accumulation apparent energy
register, are both read following the line cycle accumulation
interrupt. Figure 87 shows a flowchart for calibrating active and
apparent energy simultaneously.
VAG A IN = INT
LVA E N E RG Y
⎛
⎜
⎜
INT
VAh
⎜
constant
⎜
LSB
⎝
⎛
⎛
LVAENERGY
⎜
⎜
⎜
⎜
LVAENERGY
⎝
⎝
IB(expected)
)(
expectedIB
nominalIB
−
)(
=
×
IV
Bnominal
×
×
s/h3600
⎞
⎞
12
⎟
⎟
(69)
21
×
⎟
⎟
⎠
⎠
⎞
⎟
⎟
(70)
(s)
timeonAccumulati
⎟
⎟
⎠
The accumulation time is determined from Equation 37 and the
line period can be determined from the PERIOD register according to Equation 38. The VA h represented by the VAENERGY
register is
VA h = VAENERGY × VAh /LSB constant (71)
The VA h/ L SB constant can be verified using this equation:
Rev. A | Page 45 of 60
VAh
LSB
constant
timeonAccumulati
VA
×
=
LVAENERGY
(s)
3600
(72)
Page 46
ADE7753
CALCULATE CFDEN VALUE FOR DESIGN
WRITE CFDEN VALUE TO CFDEN REGISTER
SET HALF LINE CYCLES FOR ACCUMULATION
ADDR. 0x15 = CFDEN
SET I
= Ib, V
TEST
IN LINECYC REGISTER ADDR. 0x1C
SET MODE FOR LINE CYCLE
ACCUMULATION ADDR. 0x09 = 0x0080
ENABLE LINE CYCLE ACCUMULATION
INTERRUPT ADDR. 0x0A = 0x04
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. = 0x0C
RESET THE INTERRUPT STATUS
READ REGISTER ADDR. = 0x0C
= V
TEST
INTERRUPT?
YES
NOM
, PF = 1
NO
INTERRUPT?
YES
READ LINE ACCUMULATION ENERGY
ACTIVE ENERGY: ADDR. 0x04
APPARAENT ENERGY: ADDR. 0x07
CALCULATE WGAIN. SEE EQUATION 47.
CALCULATE VAGAIN. SEE EQUATION 69.WRITE VGAIN VALUE TO ADDR. 0x1A
NO
Figure 87. Active/Apparent Gain Calibration
Reactive Energy
Reactive energy is only available in line accumulation mode in
the ADE7753. The accumulated reactive energy over LINECYC
number of half line cycles is stored in the LVARENERGY register.
In the ADE7753, a low-pass filter at 2 Hz on the current channel
is implemented for the reactive power calculation. This provides
the 90 degree phase shift needed to calculate the reactive power.
This filter introduces 1/f attenuation in the reactive energy
accumulated. Compensation for this attenuation can be done
externally in a microcontroller. The microcontroller can use the
LVARENERGY register in order to produce a pulse output
similar to the CF pulse for reactive energy.
WRITE WGAIN VALUE TO ADDR. 0x12
02875-A-004
To create a VAR pulse, an impulse/VARh constant must be
determined. The 1/f attenuation correction factor is determined
by comparing the nominal reactive energy accumulation rate to
the expected value. The attenuation correction factor is multiplied by the contents of the LVARENERGY register, with the
ADE7753 in line accumulation mode.
Rev. A | Page 46 of 60
Page 47
ADE7753
The impulse/LSB ratio used to convert the value in t
LVARENERGY register into a pulse output can be expressed in
terms of impulses/VA
imp/LSB =
VA RC F
IB(expected)
R h and VA R h /LSB.
LSBVARhVARhimp
//=×
=
)/(
VARCF
VARCF
××
IVVARhimptVARConstan
bnominal
s/h3600
PERIODLVARENERGY
VA RC F
IB(nominal)
=
IB
××(s)
where the accumulation time is calculated from Equation 37
The line period can be determined from the PERI
the LVARENERGY register value:
VA Rh =
IBHz50
/××
PERIOD
VA R =
PERIODLSBVARhLVARENERGY
s/h3600/
PERIODtimeonAccumulati
×××(s)
The PERIOD
IB
/PERIOD factor in the preceding VAR equations
50 Hz
is the correction factor for the 1/f frequency attenuation of the
low-pass filter. The PERIOD
term refers to the line period at
50 Hz
calibration and could represent a frequency other than 50 Hz.
CLKIN FREQUENCY
In this data sheet, the characteristics of the ADE7753 are shown
when CLKIN frequency is equal to 3.579545 MHz. However, the
ADE7753 is designed to have the same accuracy at any CLKIN
frequency within the specified range. If the CLKIN frequency is
not 3.579545 MHz, various timing and filter characteristics need
to be redefined with the new CLKIN frequency. For example,
the cutoff frequencies of all digital filters such as LPF1, LPF2, or
HPF1, shift in proportion to the change in CLKIN frequency
according to the following equation:
FrequencyOriginalFrequencyNew
The change of CLKIN frequency does not affect the timing
characteristics of the serial interface because the data transfer is
synchronized with serial clock signal (SCLK). But one needs to
observe the read/write timing of the serial data transfer—see
the ADE7753 timing characteristics in Table 2. Table 9 lists
various timing changes that are affected by CLKIN frequency.
×=
579545.3
IB
PERIODtimeonAccumulati
PERIODLSBVARhLVARENERGY
FrequencyCLKIN
he
)(
expected
nominal
ϕ×
(73)
)sin(
(74)
Hz50
(7
5)
.
OD register
m according to Equation 38. Then VAR can be determined fro
(76
)
Hz50
(77)
(78)
MHz
Table 9. Frequen
cy Dependencies of the ADE7753 Parameters
Parameter CLKIN Dependency
Nyquist Frequency for CH 1 and CH 2 ADCs CLKIN/8
PHCAL Resolution (Seconds per LSB) 4/CLKIN
Active Energy Register Update Rate (Hz) CLKIN/4
Waveform Sampling Rate (per Second)
WAVSEL 1,0 = 0 0 CLKIN/128
0 1 CLKIN/256
1 0 CLKIN/512
1 1 CLKIN/1024
Maximum ZXTOUT Period 524,288/CLKIN
SUSPENDING ADE7753 FUNCTIONALITY
The analog and the digital circuit can be suspended separately.
The analog portion of the ADE7753 can be suspended by setting
the ASUSPEND bit (Bit 4) of the mode register to logic high—
see the Mode Register (0x9) section. In suspend mode, all waveform samples from the ADCs are set to 0. The digital circuitry
can be halted by stopping the CLKIN input and maintaining a
logic high or low on the CLKIN pin. The ADE7753 can be
reactivated by restoring the CLKIN input and setting the
ASUSPEND bit to logic low.
CHECKSUM REGISTER
The ADE7753 has a checksum register (CHECKSUM[5:0]) to
ensure the data bits received in the last serial read operation are
not corrupted. The 6-bit checksum register is reset before the
first bit (MSB of the register to be read) is put on the DOUT
pin. During a serial read operation, when each data bit becomes
available on the rising edge of SCLK, the bit is added to the
checksum register. In the end of the serial read operation, the
content of the checksum register is equal to the sum of all ones
in the register previously read. Using the checksum register, the
user can determine if an error has occurred during the last read
operation. Note that a read to the checksum register also
generates a checksum of the checksum register itself.
DOUT
Figure 88. Checksum Register for Serial Interface Read
CONTENT OF REGISTER (n-bytes)
+
CHECKSUM REGISTER ADDR:0x3E
+
02875-0-077
Rev. A | Page 47 of 60
Page 48
ADE7753
T
ADE7753 SERIAL INTERFACE
All ADE7753 functionality is accessible via several on-chip
registers—see Figure 89. The contents of t
updated or read using the on-chip serial interface. After poweron oe
r toggling th
RESET
pin low or a falling edge on CS, t
ADE7753 is placed in communications mode. In communications he ADects a write to its communications
mode, tE7753 exp
regisn to the communications register
ter. The data writte
determines whether the next data transfer operation
a write and also which register is accessed. Therefore all data
transfer operations with the ADE7753, whether a read or a
writa write to the communications r
e, must begin with egister.
COMMUNICATIONS
DIN
DOUT
Figure 89. Addressing ADE7753 Registers via the Communications Register
The communications reg
determines whether the n
REGISTER
REGISTER 1
REGISTER 2
REGISTER 3
REGISTER n–1
REGISTER n
ister is an 8-bit wide register. The MSB
ext data transfer operation is a read or
a write. The six LSBs contain the address of the register to be
accessed—see the Communications Register section for a more
detailed description.
Figure 90 and Figure 91 show the data transfer sequences for a
read and write operation, respectively. On completion of a data
transfer (read or write), the ADE7753 once again enters
communications mode. A data transfer is complete when the
LSB of the ADE7753 register being addressed (for a write or a
read) is transferred to or from the AD
hese registers can be
is a read or
IN
OUT
IN
OUT
OUT
OUT
OUT
IN
IN
IN
REGISTER
ADDRESS
DECODE
02875-0-078
E7753.
he
CS
SCLK
COMMUNICATIONS REGISTER WRITE
DIN
DOU
Figure 90. Reading the Serial Inter
CS
SCLK
COMMUNICATIONS REGISTER WRITE
DIN
Figure 91. Writing Data to the ADE7753 via the Serial Interface
ADDRESS00
MULTIBYTE
Data from the ADE7753 viaface
ADDRESS01
MULTIBYTE READ DA
READ DATA
02875-0-079
TA
02875-0-08
The serial interface of the ADE7753 is made up of four signals:
SCLK, DIN, D OUT, and
CS
. The serial clock for a data transfer
is applied at the SCLK logic input. This logic input has a
Schmitt-trigger input structure that allows slow rising (and
falling) clock edges to be used. All data transfer operations
are
synchronized to the serial clock. Data is shifted into the
ADE7753 at the DIN logic in
put on the falling edge of SCLK.
753 at the DOUT logic output Data is shifted out of the ADE7
CS
on a rising edge of SCLK. The
logic input is the chip-select
input. This input is used when multiple devices share the serial
bus. A falling edge on
places the ADE7753 into communications mode. The
CS
also resets the serial interface and
CS
inpu
t
should be driven low for the entire data transfer operation.
Bringing
CS
high during a data transfer operation aborts the
transfer and places the serial bus in a high impedance state. The
CS
logic input can be tied low if the ADE7753 is the only device
CS
on the serial bus. However, with
tied low, all initiated data
transfer operations must be fully completed, i.e., the LSB of each
register must be transferred because there is no other way
bringing the ADE7753 back into communications mo
without resetting the entire device by using
RESET
of
de
.
0
Rev. A | Page 48 of 60
Page 49
ADE7753
K
ADE7753 Serial Write Operation
The serial write sequence takes place as follows. With the
ADE7753 in communications mode (i.e., the
CS
input logic
low), a write to the communications register first takes place.
The MSB of this byte transfer is a 1, indicating that the data
transfer operation is a write. The LSBs of this byte contain the
address of the register to be written to. The ADE7753 starts
shifting in the register data on the next falling edge of SCL
K. All
remaining bits of register data are shifted in on the falling edge
of subsequent SCLK pulses—see Figure 92. As explained earlie
the data write is initiated by a write to the communications
register followed by the data. During a data write operation to
the ADE7753, data is transferred to all on-chip registers one
byte at a time. After a byte is transferred into the serial port,
there is a finite time before it is transferred to one of the
ADE7753 on-chip registers. Although another byte transfer to
the serial port can start while the previous byte is being
transferred to an on-chip register, this second byte transfer
CS
SCL
DIN
t
1
10
t
3
t
t
2
4
A4A5A3
t
5
A2
A0
A1
r,
t
7
should not finish until at least 4 µs after the end of the previous
byte transfer. This functionality is expressed in the timing
specification t
during a byte transfer (
—see Figure 92. If a write operation is aborted
6
CS
brought high), then that byte cannot
be written to the destination register.
Destination registers can be up to 3 bytes wide—see the
ADE
7753 Register Description tables. Therefore the first byte
shifted into the serial port at DI is transferred to the MSB
N
(most significant byte) of the destination register. If, for
example, the addressed register is 12 bits wide, a 2-byte data
transfer must take place. The data is always assumed to be right
justified, therefore in this case, the four MSBs of the first byte
would be ignored and the four LSBs of the first byte written to
the A
DE7753 would be the four MSBs of the 12-bit word.
Figure 93 illustrates this example.
t
8
t
6
t
7
B7
D
DB0
DB7
DB0
COMMAND BYTE
SCLK
DINXXXXDB11 DB10 DB9
MOST SIGNIFICANT BYTE
Figure 93. 12-Bit Serial Write Operation
MOST SIGNIFICANT BYTE
e Write Timing Figure 92. Serial Interfac
DB8
DB7 DB6DB5DB4DB3 DB2DB1 DB0
LEAST SIGNIFICANT BYTE
LEAST SIGNIFICANT BYTE
02875-0-082
02875-0-081
Rev. A | Page 49 of 60
Page 50
ADE7753
ADE7753 Serial Read Operation
During a data read operation from the ADE7753, data is sh
out at the DOUT logic output on the rising edge of SCLK. As
the case with the data write operation, a data read must be
preceded with a write to the communications register.
ifted
is
high impedance state on the falling edge of the last SCLK pulse.
CS
The read operation can be aborted by bringing the
logic
input high before the data transfer is complete. The DOUT
output enters a high impedance state on the rising edge of
CS
.
CS
With the ADE7753 in communications mode (i.e.,
logic
low), an 8-bit write to the communications register first takes
place. The MSB of this byte transfer is a 0, indicating that the
next data transfer operation is a read. The LSBs of this byte
contain the address of the register that is to be read. The
ADE7753 starts shifting out of the register data on the next
rising edge of SCLK—see Figure 94. At this point, the DOUT
logic output leaves its high impedance state and starts driving
the data bus. All remaining bits of register data are shifted ou
on subsequent SCLK rising edges. The serial interface also
enters communications mode again as soon as the read has
been completed. At this point, the DOUT logic output enters
CS
t
1
SCLK
0
DIN
DOUT
0
A4A5A3
COMMAND BYTE
A2
A1
Figure 94. Serial Interface Read Timing
When an ADE7753 register is addresse
the entire contents of that register are transferred to the s
d for a read operation,
erial
port. This allows the ADE7753 to modify its on-chip registers
without the risk of corrupting data during a multibyte transf
Note that when a read operation follows a write operation, th
er.
e
read command (i.e., write to communications register) should
t
not happen for at least 4 µs after the end of the write operation.
If the read command is sent within 4 µs of the write operation,
the last byte of the write operation could be lost. This timing
constraint is given as timing specification t
.
9
a
t
t
9
A0
t
11
DB7
MOST SIGNIFICANT BYTE
t
10
t
11
DB0
DB7
LEAST SIGNIFICANT BYTE
13
t
12
DB0
02875-0-083
Rev. A | Page 50 of 60
Page 51
ADE7753
ADE7753 REGISTERS
Table 10. Summary of Registers by Address
Address Name R/W No. Bits Default Type
0x01 WAVEFORM R 24 0x0 S
0x02 AENERGY R 24 0x0 S
0x03 RAENERGY R 24 0x0 S
0x04 LAENERGY R 24 0x0 S
0x05 VAENERGY R 24 0x0 U
0x06 RVAENERGY R 24 0x0 U
0x07 LVAENERGY R 24 0x0 U
0x08 LVARENERGY R 24 0x0 S
0x09 MODE R/W 16 0x000C U
0x0A IRQEN R/W 16 0x40 U
0x0B STATUS R 16 0x0
0x0C RSTSTATUS R 16 0x0 U
0x0D CH1OS R/W 8 0x00 S
0x0E CH2OS R/W 8 0x0 S
0x0F GAIN R/W 8 0x0 U
0x10 PHCAL R/W 6 0x0D S
0x11 APOS R/W 16 0x0 S
1
Descriptio
Waveform
data from either Channel 1, Channel 2, or the active power signal. The data
source an
Bits 14 an
Channel 2
Active Ene
in this 24-
Same as t
following
Line Accu
is accumu
line cycles
Apparent his
read-only
Same as the VAENERGY register except that the register is reset to 0
following a read operation.
Line Accumulation Apparent Energy Register. The instantaneous real
power is accumulated in this read-only register over the LINECYC number
of half line cycles.
Line Accumulation Reactive Energy Register. The instantaneous reactive
power is accumulated in this read-only register over the LINECYC number
of half line cycles.
Mode Register. This is a 16-bit register through which most of the ADE7753
functionality is accessed. Signal sample rates, filter enabling, and
calibration modes are selected by writing to this register. The contents can
be read at any time—see the Mode Register (0x9) section.
Interrupt Enable Register. ADE7753 interrupts can be deactivated at any time
by setting the corresponding bit in this 16- bit enable register to Logic 0.
The status register continues to register an interrupt event even if disabled.
However, the
section.
U
Interrupt Status Regist
register contains information regarding the source of ADE7753
interrupts—the see ADE7753 Interrupts section.
Same as the interrupt status register except that the register contents are
reset to 0 (all flags cleared) after a read operation.
*
Channel 1 Offset Adjust. Bit 6 is not used. Writing to Bits 0 to 5 allows
offsets on Channel 1 to be removed—see the Analog Inputs and CH1OS
Register (0x0D) sections. Writing a Logic 1 to the MSB of this register
enables the digital integrator on Channel 1, a Logic 0 disables the
integrator. The default value of this bit is 0.
*
Channel 2 Offset Adjust. Bits 6 and 7 are not used. Writing to Bits 0 to 5 of
this register allows any offsets on Channel 2 to be removed—see the
Analog Inputs section. Note that the CH2OS register is inverted. To apply a
positive offset, a negative number is written to this register.
PGA Gain Adjust. This 8-bit register is used to adjust the gain selection for
the PGA in Channels 1 and 2—see the Analog Inputs section.
Phase Calibration Register. The phase relationship between Channel 1 and
2 can be adjusted by writing to this 6-bit register. The valid content of this
twos compliment register is between 0x1D to 0x21. At a line frequency of
60 Hz, this is a range from –2.06° to +0.7°—see the Phase Compensation
section.
Active Power Offset Correction. This 16-bit register allows small offsets in
the active power calculation to be removed—see the Active Power
Calculation section.
n
Register. This read-only register contains the sampled waveform
d the length of the waveform registers are selected by data
d 13 in the mode register—see the Channel 1 Sampling and
Sampling sections.
rgy Register. Active power is accumulated (integrated) over time
bit, read-only register—see the Energy Calculation section.
he active energy register except that the register is reset to 0
a read operation.
mulation Active Energy Register. The instantaneous active power
lated in this read-only register over the LINCYC number of half
.
Energy Register. Apparent power is accumulated over time in t
register.
IRQ
output is not activated—see the ADE7753 Interrupts
er. This is an 16-bit read-only register. The status
Rev. A | Page 51 of 60
Page 52
ADE7753
o. Bits Default Type1Description Address Name R/W N
0x12 WGAIN R/W 12 0x0 S
0x13 WDIV R/W 8 0x0 U
0x14 CFNUM R/W 12 0x3FU
0x15 CFDEN R/W 12 0x3F U
0x16 IRMS R 24 0x0 U Channel 1 RMS Value (Current Channel).
0x17 VRMS R 24 0x0 U Channel 2 RMS Value (Voltage Channel).
0x18 IRMSOS R/W 12 0x0 S et Correction Register. Channel 1 RMS Offs
0x19 VRMSOS R/W 12 0x0 S Channel 2 RMS Offset Correction Register.
0x1A VAGAIN R/W 12 0x0 S
0x1B VADIV R/W 8 0x0 U
0x1C LINECYC R/W 16 0xFFFF U
0x1D ZXTOUT R/W 12 0xFFF U
0x1E SAGCYC R/W 8 0xFF U
0x1F SAGLVL R/W 8 0x0 U
0x20 IPKLVL R/W 8 0xFF U
0x21 VPKLVL R/W 8 0xFF U
0x22 IPEAK R 24 0x0 U
0x23 RSTIPEAK
0x24 VPEAK R 24 0x0 U
0x25 RSTVPEAK R 24 0x0 U
0x26 TEMP R 8 0x0 S
R 240x0 U
Power Gain Adjust. This is a 12-bit register. The active power calculation
can be calibrated by writing to this register. The calibration range is ±50%
of the nomin
0.0244%/LSB —see the Calibrating an Energy Meter Based on the ADE7753
section.
Active Energy Divider Register. The internal active energy register is
divided by the value of this register before being stored in the AENERG
register.
CF Frequency Divider Numerator Register. The output frequency on the CF
pin is adjusted by writing to this 12-bit read/write register—see the
Energy-to-Frequency Conversion section.
CF Frequency Divider Denominator Register. The output frequency on the
CF pin is adjusted by writing to this 12-bit read/write register—see the
Energy-to-Frequency Conversion section.
Apparent Gain Register. App
writing to this register. The calibration range is 50% of the nominal ful
scale real power. The resolution of the gain adjust is 0.02444%/LSB.
Apparent Energy D
divided by the value of this register before being stored in the VAENERGY
register.
register is used during line cycle energy accumulation mode to set the
number of half line cycles for energy accumulation—see the Line Cycle
Energy Accumulation Mode section.
within a time period specified by this 12-bit register, the interrupt request
line (
Sag Line Cycle Register. This 8-bit register specifies the number of
consecutive line cycles the signal on Channel 2 must be below SAGLVL
before th
section.
signal level on Channel 2 the
remain low for the number of cycles specified in the SAGCYC register
before the
section.
Channel 1 Peak Level Threshold (Current Channel). This register sets the
level of the current peak detection. If the Channel 1 input exceeds this
level, the PKI flag in the status register is set.
Channel 2 Peak Level Threshold (Voltage Ch
level of the voltage peak detection. If the Channel 2 input exceeds this
level, the PKV flag in the status register is set.
Channel 1 Peak Register. The maximum input value of the current channel
since the last read of the register is stored in this register.
Same as Channel 1 Peak Register except that the register contents are rese
to 0 after read.
Channel 2 Peak Register. The maximum input value of the voltage channel
since the last read of the register is stored in this register.
Same as Channel 2 Peak Register except that the register contents are rese
to 0 after a read.
Temperature Register. This is an 8-bit register which contains the result of
the latest temperature conversion—see the Temperature Measurement
section.
al full-scale active power. The resolution of the gain adjust is
arent power calculation can be calibrated by
ivider Register. The internal apparent energy register is
ccumulation Mode Line-Cycle Register. This 16-bit Line Cycle Energy A
IRQ) is activated—see the Zero-Crossing Detection section.
e SAG output is activated—see the Line Voltage Sag Detection
SAG pin becomes active. The signal must
SAG pin is activated—see the Line Voltage Sag Detection
Y
l-
Channel 2 Zero-Crossing Timeout. If no zero crossings are detected on
hat peak Sag Voltage Level. An 8-bit write to this register determines at w
annel). This register sets the
t
t
Rev. A | Page 52 of 60
Page 53
ADE7753
Address Name R/W No. Bits Default Type1Description
0x27 PERIOD R 16 0x0 U
0x28–
0x3C
0x3D TMODE R/W 8 – U e Register. Test Mod
0x3E CHKSUM R 6 0x0 U
0x3F DIEREV R 8 – U
1
Type decoder: U = unsigned, S = signed by twos complement method, and S* = signed by sign magnitude method.
Period of the Channel 2 (Voltage Channel) Input Estimated by ZeroCrossing Processing. The MSB of this register is always zero.
Reserved.
Checksum Register. This 6-bit read-only register is equal to the sum of all
the ones in the previous read—see the ADE7753 Serial Read Operation
section.
Die Revision Register. This 8-bit read-only register contains the revision
number of the silicon.
Rev. A | Page 53 of 60
Page 54
ADE7753
ADE7753 REGISTER DESCRIPTIONS
All ADE7753 functionality is accessed via the on-chip registers.ions register
en transferring the r ister data. A ful escription theface protocol is given in the ADE7753 Serial Interface section.
and thegl dof serial inter
MUONS R
COMNICATIEGISTER
omm regis is a-bit, wrily regiswh
The cunicationstern 8te-onter ich controls the serial data transfer between the ADE7753 and the host
processor. All data transfer operations must begin with a write t
regist
desig
6 RESERVED This bit is unused and should be set to 0.
7 W/R
Bit
Mnemonic Description
The six LSBs of the communications register specify the register for the data transfer operation. Table 10 lists
the address of each ADE7753 on-chip register.
When this bit is a Logic 1, the data transfer operation immediately following the write to the
communications register is interpreted as a write to the ADE7753.
When this bit is a Logic 0, the data transfer operation immediately following the write to the
communications register is interpreted as a read operation.
MODE REGISTER (0x09)
The ADE7753 functionality is configured by writing to the mode register. Table 12 describes the functionality of each bit in the register.
Each register is accessed by first writing to the communicat
o the communications register. The data written to the communications
r a ite and which register is being accessed. Table 11 outlines the bit
Table 12. Mode Register
Bit
Location
0 DISHPF 0 HPF (high-pass filter) in Channel 1 is disabled when this bit is set.
1 DISLPF2 0 LPF (low-pass filter) after the multiplier (LPF2) is disabled when this bit is set.
2 DISCF 1 Frequency output CF is disabled when this bit is set.
3 DISSAG 1 Line voltage sag detection is disabled when this bit is set.
4 ASUSPEND 0
5 TEMPSEL 0
6 SWRST 0
7 CYCMODE 0 Setting this bit to Logic 1 places the chip into line cycle energy accumulation mode.
8 DISCH1 0 ADC 1 (Channel 1) inputs are internally shorted together.
9 DISCH2 0 ADC 2 (Channel 2) inputs are internally shorted together.
10 SWAP 0
12, 11 DTRT1, 0 00
Bit
Mnemonic
Default
Value
Description
By setting this bit to Logic 1, both ADE7753 A/D converters can be turned off. In normal
operation, this bit should be left at Logic 0. All digital functionality can be stopped by suspending
the clock signal at CLKIN pin.
Temperature conversion starts when this bit is set to 1. This bit is automatically reset to 0 when
the temperature conversion is finished.
Software Chip Reset. A data transfer should not take place to the ADE7753 for at least 18 µs after a
software reset.
By setting this bit to Logic 1 the analog inputs V2P and V2N are connected to ADC 1 and the
analog inputs V1P and V1N are connected to ADC 2.
These bits are used to select the waveform register update rate.
DTRT 1 DTRT0 Update Rate
0 0 27.9 kSPS (CLKIN/128)
0 1 14 kSPS (CLKIN/256)
1 0 7 kSPS (CLKIN/512)
1 1 3.5 kSPS (CLKIN/1024)
Rev. A | Page 54 of 60
Page 55
ADE7753
Bit
Location
14, 13
15 POAM 0 Writing Logic 1 to this bit allows only positive power to be accumulated in the ADE7753.
(WAVEFORM SELECTION FOR SAMPLE MODE)
(SHORT THE ANALOG INPUTS ON CHANNEL 2)
(SHORT THE ANALOG INPU
Bit
Mnemonic
WAVSEL1, 0 00
TIVE ONLY AC MULATION)
(POSICU
(WAVEFORPLES OUTPU
M SAM
00 = 27.9kSP
01 = 14.4kSP
10 = 7.2kSP
11 = 3.6kSP
(SWAP CH1 AND CH2 ADCs)
TS ON CHANNEL 1)
Default
Value
PO
WAVSEL
00 = LPF2
01
= RESERVED
10 = CH1
11 = CH2
T DATA RATE)
S (CLKIN/128)
S (CLKIN/256)
S (CLKIN/512)
S (CLKIN/1024)
SWAP
DISCH2
DISCH1
Description
These bits are used to select the source of the sampled data for the waveform register.
WAVSEL1, 0 Length Source
0 0 24 bits active power signal (output of LPF2)
0 1 Reserved
1 0 24 bits Channel 1
1 1 24 bits Channel 2
15 14 13 12 11 10 9 8 7 6 5 4 3 2 1 0
0000000000001100
AM
DTRT
ADDR: 0x09
DISHPF
(DISABLE HPF1 IN CHANNEL 1)
DISLPF2
(DISABLE LPF2 AFTER MULTIPLIER)
DISCF
(DISABLE FREQUENCY OUTPUT CF)
DISSAG
(DISABLE SAG OUTPUT)
ASUSPEND
(SUSPEND CH1 AND CH2 ADCs)
TEMPSEL
(START TEMPERATURE SENSING)
SWRST
(SOFTWARE CHIP RESET)
CYCMODE
(LINE CYCLE ENERGY ACCUMULATION MODE)
NOTE: REG
ISTER CONTENTS SHOW POWER-ON DEFAULTS
Figure 95. Mode Register
02875-0-084
Rev. A | Page 55 of 60
Page 56
ADE7753
)
INTERRU
RESET IN
INTERT ENABLE EGIx0A)
The status register is used by the MCU toe source orupt req
ADE7753, the corresponding flag in the irrupt status register it to logic highe interrupt
enable register, the
interrupt status register to determine the rce of the interrupt.
P R (0
T STATUS
TTAEGI,
ERRUPT S
EGISTER
TUS R
x0B),
STER (0x0C)
RUPRSTER (0
determine thf an interuest (
ntes se. If the ena
IRQ
logic output goes active low. When the MCU services the irupt, it must first carry out a read from the
sou
nter
IRQ
). When an interrupt event occurs
ble bit for this flag is Logic 1 in th
in the
Table 13. Interrupt Status Register, Reseterrupt Status Register, and Interrup
Bit Interru
ocation
L
0 AEHF
pt
Flag Description
Indicates that an interrupt was caused by the 0-to-1 transition of the MSB of the active energy register, i.e., the
t Int Enable Register
AENERGY register is half full.
1 SAG Indicates that an interrupt was caused by a SAG on the line voltage.
2 CYCEND
Indicates the end of energy accumulation over an integer number of half line cycles as defined by the content
of the LINECYC register—see the Line Cycle Energy Accumulation Mode section.
3 WSMP Indicates that new data is present in the waveform register.
4 ZX This status bit reflects the status of the ZX logic ouput—see the Zero-Crossing Detection section.
5 TEMP Indicates that a temperature conversion result is available in the temperature register.
6 RESET
Indicates the end of a reset (for both software or hardware reset). The corresponding enable bit has no
function in the interrupt enable register, i.e., this status bit is set at the end of a reset, but it cannot be enabled
to cause an interrupt.
7 AEOF Indicates that the active energy register has overflowed.
8 PKV Indicates that waveform sample from Channel 2 has exceeded the VPKLVL value.
9 PKI Indicates that waveform sample from Channel 1 has exceeded the IPKLVL value.
A VAEHF
Indicates that an interrupt was caused by the 0 to 1 transition of the MSB of the apparent energy register, i.e.,
the VAENERGY register is half full.
B VAEOF Indicates that the apparent energy register has overflowed.
C ZXTO
Indicates that an interrupt was caused by a missing zero crossing on the line voltage for the specified number
of line cycles—see the Zero-Crossing Timeout section.
D PPOS Indicates that the power has gone from negative to positive.
E PNEG Indicates that the power has gone from positive to negative.
F RESERVED Reserved.
The CH1OS register is an 8-bit, read/write enabled register
Channel 1, and Bits 0 to 5 indicates the amount o
f the offset correction in Channel 1. Table 14 summarizes the function of this register.
Table 14. CH1OS Register
Bit
Location
0 to 5 OFFSET
Bit
Mnemonic Description
The six LSBs of the CH1OS register control the amount of dc offset correction in Channel 1 ADC. The 6-bit
offset correction is sign and magnitude coded. Bits 0 to 4 indicate the magnitude of the offset correction.
Bit 5 shows the sign of the offset correction. A 0 in Bit 5 means the offset
indicates the offset correction is negative.
6 Not Used used. This bit is un
7 INTEGRATOR
This bit is used to activate the digital integrator on Channel 1. The digital integrator is switched on by setting
this bit. This bit is set to be 0
DIGITAL INTEGRATOR SELECTION
1 = ENABLE
0 = DISABLE
NOT USED
. The MSB of this register is used to switch on/off the digital integrator in
correction is positive and a 1
on default.
76543210
00000000
Figure 97. Channel 1 Offset Register
ADDR: 0x0D
SIGN AND MAGNITUDE CODED
OFFSET CORRECTION BITS
02875-0-086
Rev. A | Page 57 of 60
Page 58
ADE7753
S OUTLINE DIMENSION
2.00 MAX
0.05 MIN
COPLANARITY
0.10
Figure 98. 20-Lead Shrink Small Outline Package [SSOP]
7.50
7.20
6.90
2011
5.60
5.30
8.20
5.00
0.25
0.09
SEATING
PLANE
7.80
7.40
8°
4°
0°
1
0.65
BSC
COMPLIANT TO JEDEC STANDARDS MO-150AE
1.85
1.75
1.65
0.38
0.22
10
0.95
0.75
0.55
ORDERING GUIDE
Model Package Description Package Option Temperature Range
ADE7753ARS 20-Lead SSOP RS-20 −40°C to +85°C
ADE7753ARSRL 20-Lead SSOP RS-20 −40°C to +85°C
ADE7753ARSZ
ADE7753ARSZRL1 20-Lead SSOP RS-20 −40°C to +85°C
EVAL-ADE7753EB Evaluation Board