High accuracy active energy measurement IC, supports
IEC 687/61036
Less than 0.1% error over a dynamic range of 500 to 1
Supplies active power on the frequency outputs F1 and F2
High frequency output CF is intended for calibration and
supplies instantaneous active power
Continuous monitoring of the phase and neutral current
allows fault detection in 2-wire distribution systems
Current channels input level best suited for current
transformer sensors
Uses the larger of the two currents (phase or neutral) to
bill—even during a fault condition
Continuous monitoring of the voltage and current inputs
allows missing neutral detection
Uses one current input (phase or neutral) to bill when
missing neutral is detected
Two logic outputs (FAULT and REVP) can be used to indicate
a potential miswiring, fault, or missing neutral condition
Direct drive for electromechanical counters and 2-phase
stepper motors (F1 and F2)
Proprietary ADCs and DSP provide high accuracy over large
variations in environmental conditions and time
Reference 2.5 V ± 8% (drift 30 ppm/°C typical) with external
overdrive capability
Single 5 V supply, low power
FUNCTIONAL BLOCK DIAGRAM
AGNDFAULT
V
2
MISCA
1A
V
1N
V
1B
V
2P
V
2N
4
3
7
6
5
2.5V
REFERENCE
4kΩ
ADC
ADC
ADC
ADC
A>B
B>A
A<>B
MISSING NEUTRAL
INTERNAL
OSCILLATOR
HPF
GAIN ADJUST
Fault and Missing Neutral Detection
ADE7761
GENERAL DESCRIPTION
The ADE7761 is a high accuracy, fault tolerant, electrical energy
measurement IC intended for use with 2-wire distribution
systems. The part specifications surpass the accuracy requirements as quoted in the IEC61036 standard.
The only analog circuitry used on the ADE7761 is in the ADCs
and reference circuit. All other signal processing (such as multiplication and filtering) is carried out in the digital domain. This
approach provides superior stability and accuracy over extremes
in environmental conditions and over time.
The ADE7761 incorporates a fault detection scheme similar to
the ADE7751 by continuously monitoring both the phase and
neutral currents. A fault is indicated when these currents differ
by more than 6.25%.
(continued on Page 3)
V
1518
ZERO CROSSING
DETECTION
MISSING NEUTRAL
DETECTION
DIGITAL-TO-FREQUENCY CONVERTER
DD
POWER
SUPPLY MONITOR
ADE7761
SIGNAL PROCESSING
BLOCK
LPF
91417101112
IN/OUT
16181920
F1F2CFREVPS0S1SCFDGNDRCLKINREF
04407-0-001
Figure 1.
Rev. A
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.
Changes to Ordering Guide.......................................................... 25
1/04—Revision 0: Initial Version
Rev. A | Page 2 of 28
ADE7761
GENERAL DESCRIPTION
(continued from Page 1)
The ADE7761 incorporates a missing neutral detection scheme
by continuously monitoring the input voltage. When a missing
neutral condition is detected—no voltage input—the ADE7761
continues billing based on the active current signal (see the
Missing Neutral Mode section). The missing neutral condition
is indicated when the FAULT pin goes high.
The ADE7761 supplies average active power information on the
low frequency outputs F1 and F2. The CF logic output gives
instantaneous active power information.
The ADE7761 includes a power supply monitoring circuit on
that the voltage and current channels are matched. An internal
no-load threshold ensures that the ADE7761 does not exhibit
any creep when there is no load.
Rev. A | Page 3 of 28
ADE7761
SPECIFICATIONS
VDD = 5 V ± 5%, AGND = DGND = 0 V, on-chip reference, on-chip oscillator, T
Table 1.
Parameter Value Unit Test Conditions/Comments
ACCURACY1
Measurement Error2 0.1 % of reading, typ Over a dynamic range of 500 to 1
Phase Error between Channels
(PF = 0.8 Capacitive) ±0.05 Degrees, max Phase lead 37°
(PF = 0.5 Inductive) ±0.05 Degrees, max Phase lag 60°
AC Power Supply Rejection2
Output Frequency Variation 0.01 %, typ V1A = V1B = V2P = ±100 mV rms
DC Power Supply Rejection2
Output Frequency Variation 0.01 %, typ V1A = V1B = V2P = ±100 mV rms
FAULT DETECTION
2, 3
See the Fault Detection section
Fault Detection Threshold
Inactive Input <> Active Input 6.25 %, typ (V1A or V1B active)
Input Swap Threshold
Inactive Input <> Active Input 6.25 % of larger, typ (V1A or V1B active)
Accuracy Fault Mode Operation
V1A Active, V1B = AGND 0.1 % of reading, typ Over a dynamic range of 500 to 1
V1B Active, V1A = AGND 0.1 % of reading, typ Over a dynamic range of 500 to 1
Fault Detection Delay 3 Seconds, typ
Swap Delay 3 Seconds, typ
V1A Active, V1B = V2P = AGND 0.1 % of reading, typ Over a dynamic range of 500 to 1
V1B Active, V1A = V2P = AGND 0.1 % of reading, typ Over a dynamic range of 500 to 1
Missing Neutral Detection Delay 3 Seconds, typ
ANALOG INPUTS V1A − V1N, V1B − V1N, V2P − V2N
Maximum Signal Levels ±660 mV peak, max Differential input
660 mV peak, max Differential input MISCAL − V2N
Input Impedance (DC) 400 kΩ, min
Bandwidth (−3 dB) 7 kHz, typ
ADC Offset Error2 10 mV, max Uncalibrated error, see the Terminology section for details
Gain Error ±4 %, typ External 2.5 V reference
REFERENCE INPUT
REF
Input Voltage Range 2.7 V, max 2.5 V + 8%
IN/OUT
2.3 V, min 2.5 V − 8%
Input Impedance 4 kΩ, min
Input Capacitance 10 pF, max
ON-CHIP REFERENCE
Reference Error ±200 mV, max
Temperature Coefficient 30 ppm/°C, typ
Current Source 20 µA, min
ON-CHIP OSCILLATOR
Oscillator Frequency 450 kHz
Oscillator Frequency Tolerance ±12 % of reading, typ
Temperature Coefficient 30 ppm/°C, typ
See footnotes on next page.
MIN
to T
= –40°C to +85°C.
MAX
Rev. A | Page 4 of 28
ADE7761
Parameter Value Unit Test Conditions/Comments
LOGIC INPUTS5
SCF, S1, and S0
Input High Voltage, V
Input Low Voltage, V
Input Current, IIN ±3 µA, max Typical 10 nA, VIN = 0 V to VDD
Input Capacitance, CIN 10 pF, max
LOGIC OUTPUTS5
CF, REVP, and FAULT
Output High Voltage, VOH 4 V, min VDD = 5 V ± 5%
Output Low Voltage, VOH 1 V, max VDD = 5 V ± 5%
F1 and F2
Output High Voltage, VOH 4 V, min VDD = 5 V ± 5%, I
Output Low Voltage, VOH 1 V, max VDD = 5 V ± 5%, I
POWER SUPPLY For specified performance
VDD 4.75 V, min 5 V − 5%
5.25 V, max 5 V + 5%
VDD 4 mA, max
1
See plots in the Typical Performance Characteristics section.
2
See the Terminology section for explanation of specifications.
3
See the Fault Detection section for explanation of fault detection functionality.
4
See the Missing Neutral Detection section for explanation of missing neutral detection functionality.
5
Sample tested during initial release and after any redesign or process change that may affect this parameter.
2.4 V, min VDD = 5 V ± 5%
INH
0.8 V, max VDD = 5 V ± 5%
INL
SOURCE
= 10 mA
SINK
= 10 mA
Rev. A | Page 5 of 28
ADE7761
C
TIMING CHARACTERISTICS
VDD = 5 V ± 5%, AGND = DGND = 0 V, on-chip reference, on-chip oscillator, T
Sample tested during initial release and after any redesign or process change that may affect this parameter.
See Figure 2.
Table 2.
Parameter Value Unit Test Conditions/Comments
1
t
120 ms F1 and F2 Pulse Width (Logic High).
1
t2 See Table 6 s Output Pulse Period. See the Transfer Function section.
t3 1/2 t2 s Time between F1 Falling Edge and F2 Falling Edge.
1
t
90 ms CF Pulse Width (Logic High).
4
t5 See Table 7 s CF Pulse Period. See the Transfer Function section.
t6 CLKIN/4 s Minimum Time between F1 and F2 Pulse.
1
The pulse widths of F1, F2, and CF are not fixed for higher output frequencies. See the Transfer Function section.
to T
MIN
t
1
F1
t
6
t
2
t
F2
t
4
F
3
t
5
Figure 2. Timing Diagram for Frequency Outputs
= –40°C to +85°C.
MAX
04407-0-002
Rev. A | Page 6 of 28
ADE7761
ABSOLUTE MAXIMUM RATINGS
TA = 25°C, unless otherwise noted.
Table 3.
Parameter Rating
VDD to AGND −0.3 V to +7 V
Analog Input Voltage to AGND
, V
V
Reference Input Voltage to AGND −0.3 V to VDD + 0.3 V
Digital Input Voltage to DGND −0.3 V to VDD + 0.3 V
Digital Output Voltage to DGND −0.3 V to VDD + 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 s) 215°C
Infrared (15 s) 220°C
, V1N, V2N, V2P, MISCAL
1AP
1BP
−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; functional operation of the device at these or any
other conditions above those listed in the operational sections
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 7 of 28
ADE7761
r
e
TERMINOLOGY
Measurement Error
The error associated with the energy measurement made by the
ADE7761 is defined by the following formula:
Erro
Percentag
⎛
⎜
⎜
⎝
Phase Error between Channels
The high-pass filter (HPF) in the current channel has a phase
lead response. To offset this phase response and equalize the
phase response between channels, a phase correction network is
also placed in the current channel. The phase correction network ensures a phase match between the current channels and
voltage channels to within ±0.1° over a range of 45 Hz to 65 Hz
and ±0.2° over a range 40 Hz to 1 kHz.
Power Supply Rejection
This quantifies the ADE7761 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/100 Hz) signal is introduced onto the
supplies. Any error introduced by this ac signal is expressed as a
percentage of reading (see the Measurement Error definition
above).
=
⎞
7761
EnergyTrue
EnergyTrueADEbyregisteredEnergy
−
×
⎟
%100
⎟
⎠
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 power supplies are varied ±5%. Any error
introduced is again expressed as a percentage of reading.
ADC Offset Error
This refers to 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 input range selection (see the
Typical Performance Characteristics section). However, when
HPFs are switched on, the offset is removed from the current
channels and the power calculation is not affected by this offset.
Gain Error
The gain error in the ADE7761 ADCs is defined as the difference between the measured output frequency (minus the offset)
and the ideal output frequency. The difference is expressed as a
percentage of the ideal frequency, which is obtained from the
transfer function (see the Transfer Function section).
Rev. A | Page 8 of 28
ADE7761
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
1
Table 4. Pin Function Descriptions
Pin No. Mnemonic Description
1 VDD
Power Supply. This pin provides the supply voltage for the digital circuitry in the ADE7761. The supply
voltage should be maintained at 5 V ± 5% for specified operation. This pin should be decoupled with a
10 µF capacitor in parallel with a ceramic 100 nF capacitor.
2, 3 V1A, V1B
Analog Inputs for Channel 1 (Current Channel). These inputs are fully differential voltage inputs with
maximum differential input signal levels of ±660 mV with respect to V
maximum signal level at these pins is ±1 V with respect to AGND. Both inputs have internal ESD
protection circuitry, and an overvoltage of ±6 V can also be sustained on these inputs without risk of
permanent damage.
4 V1N
Negative Input Pin for Differential Voltage Inputs V
±1 V with respect to AGND. The input has internal ESD protection circuitry, and an overvoltage of ±6 V
can also be sustained on these inputs without risk of permanent damage. The input should be directly
connected to the burden resistor and held at a fixed potential,that is, AGND. See the Analog Inputs
section.
5 V2N
Negative Input Pin for Differential Voltage Inputs V
±1 V with respect to AGND. The input has internal ESD protection circuitry, and an overvoltage of ±6 V
can also be sustained on these inputs without risk of permanent damage. The input should be held at a
fixed potential, that is, AGND. See the Analog Inputs section.
6 V2P
Analog Inputs for Channel 2 (Voltage Channel). This input is fully differential voltage input with
maximum differential input signal levels of ±660 mV with respect to V
maximum signal level at these pins is ±1 V with respect to AGND. This input has internal ESD protection
circuitry, and an overvoltage of ±6 V can also be sustained on these inputs without risk of permanent
damage.
7 MISCAL
Analog Input for Missing Neutral Calibration. This pin can be used to calibrate the CF-F1-F2 frequencies
in the missing neutral condition. This input is fully differential voltage input with maximum differential
input signal levels of +660 mV with respect to V
this pin is ±1 V with respect to AGND. This input has internal ESD protection circuitry, and an
overvoltage of ±6 V can also be sustained on these inputs without risk of permanent damage.
8 AGND
This pin provides the ground reference for the analog circuitry in the ADE7761, that is, ADCs and
reference. This pin should be tied to the analog ground plane of the PCB. The analog ground plane is the
ground reference for all analog circuitry such as antialiasing filters, and current and voltage transducers.
For good noise suppression, the analog ground plane should be connected only to the digital ground
plane at the DGND pin.
9 REF
IN/OUT
This pin provides access to the on-chip voltage reference. The on-chip reference has a nominal value of
2.5 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 and 100 nF ceramic capacitor.
10 SCF
Select Calibration Frequency. This logic input is used to select the frequency on the calibration output
CF. Table 6 shows how the calibration frequencies are selected.
11, 12 S1, S0
These logic inputs are used to select one of four possible frequencies for the digital-to-frequency
conversion. This offers the designer greater flexibility when designing the energy meter. See the
Selecting a Frequency for an Energy Meter Application section.
V
DD
2
V
1A
V
3
1B
V
4
1N
5
2N
6
2P
7
8
9
10
ADE7761
TOP VIEW
(Not to Scale)
MISCAL
REF
V
V
AGND
IN/OUT
SCF
Figure 3. Pin Configuration (SSOP)
20
19
18
17
16
15
14
13
12
11
F1
F2
CF
DGND
REVP
FAULT
RCLKIN
INT
S0
S1
04407-0-003
for specified operation. The
1N
and V1B. The maximum signal level at this pin is
1A
and MISCAL. The maximum signal level at this pin is
2P
for specified operation. The
2N
for specified operation. The maximum signal level at
2N
Rev. A | Page 9 of 28
ADE7761
Pin No. Mnemonic Description
13 INT This pin is internally used and should be connected to DGND.
14 RCLKIN
15 FAULT
16 REVP
17 DGND
18 CF
19, 20 F2, F1
To enable the internal oscillator as a clock source on the chip, a precise low temperature drift resistor at
nominal value of 6.2 kΩ must be connected from this pin to DGND.
This logic output goes active high when a fault or missing neutral condition occurs. A fault is defined as
a condition under which the signals on V
condition is defined when the chip is powered up with no voltage at the input. The logic output is reset
to zero when a fault or missing neutral condition is no longer detected. See the Fault Detection section
and the Missing Neutral Mode section.
This logic output goes logic high when negative power is detected, that is, when the phase angle
between the voltage and current signals is greater than 90°. This output is not latched and is reset when
positive power is once again detected. The output goes high or low at the same time as a pulse is issued
on CF.
This pin provides the ground reference for the digital circuitry in the ADE7761, that is, multiplier, filters,
and digital-to-frequency converter. This pin should be tied to the digital ground plane of the PCB. The
digital ground plane is the ground reference for all digital circuitry such as counters (mechanical and
digital), MCUs, and indicator LEDs. For good noise suppression, the analog ground plane should be
connected only to the digital ground plane at the DGND pin.
Calibration Frequency Logic Output. The CF logic output, active high, gives instantaneous active power
information. This output is intended to be used for operational and calibration purposes. See the Digitalto-Frequency Conversion section.
Low Frequency Logic Outputs. F1 and F2 supply average active power information. The logic outputs
can be used to directly drive electromechanical counters and 2-phase stepper motors.
and V1B differ by more than 6.25%. A missing neutral
1A
Rev. A | Page 10 of 28
ADE7761
TYPICAL PERFORMANCE CHARACTERISTICS
1.0
PF = 1
ON-CHIP REFERENCE
–0.2
% ERROR
–0.4
–0.6
–0.8
–1.0
0.8
0.6
0.4
0.2
0
CURRENT (% of Full Scale)
–40°C
+25°C
+85°C
Figure 4. Active Power Error as a Percentage of Reading with
Internal Reference
1.5
PF = 0.5
ON-CHIP REFERENCE
% ERROR
–0.5
1.0
0.5
0
–40°C; PF = 0.5
+25°C; PF = 1
+85°C; PF = 0.5
+25°C; PF = 0.5
100.00.11.010.0
04407-0-037
1.0
PF = 1
ON-CHIP REFERENCE
–0.2
% ERROR
–0.4
–0.6
–0.8
–1.0
0.8
0.6
0.4
0.2
0
5.25V
5.00V
4.75V
CURRENT (% of Full Scale)
Figure 6. Active Power Error as a Percentage of Reading
over Power Supply with Internal Reference
2.0
ON-CHIP REFERENCE
1.5
% ERROR
–0.5
–1.0
–1.5
1.0
0.5
0
+25°C
+85°C
–40°C
100.00.11.010.0
04434-0-039
–1.0
CURRENT (% of Full Scale)
Figure 5. Active Power Error as a Percentage of Reading over
Power Factor with Internal Reference
100.00.11.010.0
04407-0-038
–2.0
CURRENT (% of Full Scale)
100.00.11.010.0
04434-0-040
Figure 7. Ampere Hour Error as a Percentage of Reading in
Missing Neutral Mode with Internal Reference
Rev. A | Page 11 of 28
ADE7761
+
10µF
RB
RB
560kΩ
100kΩ
1kΩ
33nF
1kΩ
33nF
1kΩ
33nF
1kΩ
33nF
33nF
220V
40A TO 80mA
I
RB = 18Ω
1MΩ
33nF1kΩ
100nF
2
3
4
5
6
6
V
DD
1
V
DD
V
1A
V
1B
V
1N
V
2N
V
2P
MISCAL
ADE7761
AGND DGNDINT
RCLKIN
REF
CF
FAULT
S0
S1
SCF
IN/OUT
17138
2kΩ
18
2kΩ
15
6.2kΩ
14
PS2501-1
1
2
4
3
TO FREQ.
COUNTER
10kΩ
12
11
10
9
100nF
+
10µF
04407-0-036
Figure 8. Test Circuit for Performances Curves
Rev. A | Page 12 of 28
ADE7761
-
–
OPERATION
POWER SUPPLY MONITOR
The ADE7761 contains an on-chip power supply monitor. The
power supply (V
) is continuously monitored by the ADE7761.
DD
If the supply is less than 4 V ± 5%, the ADE7761 goes into an
inactive state, that is, no energy is accumulated and the CF, F1,
and F2 outputs are disabled. 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. This
gives a high degree of immunity to false triggering due to noisy
supplies.
The power supply and decoupling for the part should be such
that the ripple at V
does not exceed 5 V ± 5% as specified for
DD
normal operation.
V
DD
5V
4V
ADE7761
REVP - FAULT - CF
F1 - F2 OUTPUTS
0V
INACTIVEACTIVE
Figure 9. On-Chip Power Supply Monitoring
TIME
INACTIVE
ANALOG INPUTS
Channel V1 (Current Channel)
The voltage outputs from the current transducers are connected
to the ADE7761 here. Channel V1 has two voltage inputs, V
and V
. These inputs are fully differential with respect to V1N.
1B
However, at any one time, only one is selected to perform the
power calculation (see the Fault Detection section).
The maximum peak differential signal on V
1A–V1N
and V1B–V1N
is ±660 mV.
Figure 10 shows the maximum signal levels on V
, V1B, and V1N.
1A
The differential voltage signal on the inputs must be referenced
to a common mode (usually AGND).
V
1A
V1
V
1N
V1
V
1B
+660mV + V
–660mV + V
DIFFERENTIAL INPUT A
V
, V
1A
1B
CM
V
CM
CM
±660mV MAX PEAK
COMMON MODE
±100mV MAX
AGND
DIFFERENTIAL INPUT B
±660mV MAX PEAK
V
CM
Figure 10. Maximum Signal Levels, Channel 1
1A
04407-0-010
04407-0-011
Channel V2 (Voltage Channel)
The output of the line voltage transducer is connected to the
ADE7761 at this analog input. Channel V2 is a single-ended
voltage input. The maximum peak differential signal on
Channel 2 is ±660 mV with respect to V
. Figure 11 shows the
2N
maximum signal levels that can be connected to Channel 2.
+660mV + V
660mV + V
V2
CM
V
CM
CM
DIFFERENTIAL INPUT
±660mV MAX PEAK
COMMON MODE
±100mV MAX
Figure 11. Maximum Signal Levels, Channel 2
V
2P
V2
V
2N
V
CM
The differential voltage V2P–V2N must be referenced to a
common mode (usually AGND). The analog inputs of the
ADE7761 can be driven with common-mode voltages of up to
100 mV with respect to AGND. However, the best results are
achieved using a common mode equal to AGND.
MISCAL Input
The input for the power calibration in missing neutral mode is
connected to the ADE7761 at this analog input. MISCAL is a
single-ended voltage input. It is recommended to use a dc signal
derived from the voltage reference to drive this pin. The maximum peak differential signal on MISCAL is +660 mV with
respect to V
. Figure 12 shows the maximum signal levels that
2N
can be connected to the MISCAL pin.
+660mV + V
MISCAL
CM
V
CM
DIFFERENTIAL INPUT
±660mV MAX PEAK
COMMON MODE
±100mV MAX
Figure 12. Maximum Signal Levels, MISCAL
MISCAL
MISCAL
V
CM
AGND
V
2N
The differential voltage MISCAL–V2N must be referenced to a
common mode (usually AGND). The analog inputs of the
ADE7761 can be driven with common-mode voltages of up to
100 mV with respect to AGND. However, best results are
achieved using a common mode equal to AGND.
Typical Connection Diagrams
Figure 13 shows a typical connection diagram for Channel V1.
The analog inputs are being used to monitor both the phase
and neutral currents. Because of the large potential difference
between the phase and neutral, two current transformers (CTs)
must be used to provide the isolation. Note that both CTs are
referenced to analog ground (AGND); the common-mode
04407-0-012
04407-0-013
Rev. A | Page 13 of 28
ADE7761
voltage, therefore, is 0 V. The CT turns ratio and burden resistor
(RB) are selected to give a peak differential voltage of ±660 mV.
Figure 14 shows two typical connections for Channel V2. The
first option uses a potential transformer (PT) to provide
complete isolation from the main voltage. In the second option,
the ADE7761 is biased around the neutral wire, and a resistor
divider is used to provide a voltage signal that is proportional to
the line voltage. Adjusting the ratio of RA and RB + VR is a
convenient way of carrying out a gain calibration on the meter.
Figure 15 shows a typical connection for MISCAL input. The
voltage reference input (REF
set the MISCAL voltage. Adjusting the level of MISCAL to
calibrate the meter in missing neutral mode can be done by
changing the ratio of RC and RD + VR
reference is used, the values of RC, RD, and VR
to limit the current sourced by the internal reference sourcing
current to below the specified 20 µA. Therefore, because V
internal = 2.5 V, RC + RD + VR
CT
RB
INIP
AGND
RB
PHASE
REF
CT
NEUTRAL
Figure 13. Typical Connection for Channel 1
±660mV
NEUTRAL
PHASE
RA*
NEUTRAL
PHASE
*RB + VR = RF
AGND
RB*
VR*
Figure 14. Typical Connection for Channel 2
IN/OUT
RC
RD
VR1
Figure 15. Typical Connection for MISCAL
) is used as a dc reference to
IN/OUT
. When the internal
1
must be chosen
1
> 600 kΩ.
1
R
F
R
F
R
R
C
F
R
C
F
R
V
1A
C
F
V
1N
C
F
V
1B
V
2P
F
C
F
V
2N
F
C
F
V
2P
V
2N
F
C
T
MISCAL
V
F
2N
C
F
REF
04407-0-015
04407-0-016
04407-0-014
INTERNAL OSCILLATOR
The nominal internal oscillator frequency is 450 kHz when
used with the recommended R
resistor value of 6.2 kΩ
OSC
between RCLKIN and DGND (see Figure 16).
The internal oscillator frequency is inversely proportional to the
value of this resistor. Although the internal oscillator operates
when used with a R
resistor value between 5 kΩ and 12 kΩ, it
OSC
is recommended to choose a value within the range of the
nominal value.
The output frequencies on CF, F1, and F2 are directly proportional to the internal oscillator frequency; therefore, the resistor
R
must have a low tolerance and low temperature drift. A low
OSC
tolerance resistor limits the variation of the internal oscillator
frequency. Small variation of the clock frequency and consequently of the output frequencies from meter to meter
contributes to a smaller calibration range of the meter. A low
temperature drift resistor directly limits the variation of the
internal clock frequency over temperature. The stability of the
meter to external variation is then better ensured by design.
ADE7761
4k
Ω
IN/OUT
9
INTERNAL
OSCILLATOR
1417
R
OSC
DGNDRCLKINREF
Figure 16. Internal Oscillator Connection
04407-0-017
2.5V
REFERENCE
ANALOG-TO-DIGITAL CONVERSION
The analog-to-digital conversion in the ADE7761 is carried out
using second-order Σ-Δ ADCs. Figure 17 shows a first-order
(for simplicity) Σ-Δ ADC. The converter is made up of two
parts: the Σ-Δ modulator and the digital low-pass filter.
MCLK
ANALOG
LOW-PASS FILTER
R
C
INTEGRATOR
∫
V
REF
1-BIT DAC
Figure 17. First-Order Σ-∆ ADC
A Σ-Δ modulator converts the input signal into a continuous
serial stream of 1s and 0s at a rate determined by the sampling
clock. In the ADE7761, the sampling clock is equal to CLKIN.
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
LATCHED
COMPARATOR
....10100101....
DIGITAL
LOW-PASS FILTER
124
04407-0-019
Rev. A | Page 14 of 28
ADE7761
S
S
)
output (and, therefore, the bit stream) approaches 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-Δ converter uses two techniques to achieve high
resolution from what is essentially a 1-bit conversion technique.
The first is oversampling, which means that the signal is
sampled at a rate (frequency) that is many times higher than the
bandwidth of interest. For example, the sampling rate in the
ADE7761 is CLKIN (450 kHz) and the band of interest is 40 Hz
to 1 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 18).
However, oversampling alone is not an efficient enough method
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. This is what happens in the Σ-Δ 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 also shown in Figure 18.
ANTIALIAS FILTER (RC
IGNAL
NOISE
01kHz225kHz450kHz
IGNAL
NOISE
01kHz225kHz450kHz
DIGITAL FILTER
FREQUENCY (Hz)
HIGH RESOLUTION
OUTPUT FROM
DIGITAL LFP
FREQUENCY (Hz)
Figure 18. Noise Reduction Due to Oversampling and
Noise Shaping in the Analog Modulator
SAMPLING FREQUENCY
SHAPED NOISE
04407-0-020
Antialias Filter
Figure 18 also shows an analog low-pass filter (RC) on input to
the modulator. This filter is present to prevent aliasing. Aliasing
is an artifact of all sampled systems, which means that frequency components in the input signal to the ADC that are
higher than half the sampling rate of the ADC appear in the
sampled signal frequency below half the sampling rate.
Figure 19 illustrates the effect.
In Figure 19, frequency components (arrows shown in black)
above half the sampling frequency (also known as the Nyquist
frequency), that is, 225 kHz, are imaged or folded back down
below 225 kHz (arrows shown in gray). This happens with all
ADCs no matter what the architecture. In the example shown,
only frequencies near the sampling frequency (450 kHz) move
into the band of interest for metering (40 Hz to 1 kHz). This
fact allows the use of a very simple low-pass filter to attenuate
these frequencies (near 250 kHz) and thereby prevent distortion
in the band of interest. A simple RC filter (single pole) with a
corner frequency of 10 kHz produces an attenuation of
approximately 33 dB at 450 kHz (see Figure 19). This is
sufficient to eliminate the effects of aliasing.
ANTIALIASING EFFECTS
SAMPLING
IMAGE
FREQUENCIES
01kHz225kHz450kHz
FREQUENCY (Hz)
Figure 19. ADC and Signal Processing in Current Channel or Voltage Channel
FREQUENCY
04407-0-021
ACTIVE POWER CALCULATION
The ADCs digitize the voltage signals from the current and
voltage transducers. A high-pass filter in the current channel
removes any dc component from the current signal. This
eliminates any inaccuracies in the active power calculation due
to offsets in the voltage or current signals (see the HPF and
Offset Effects section).
The active power calculation is derived from the instantaneous
power signal. The instantaneous power signal is generated by a
direct multiplication of the current and voltage signals. To
extract the active power component (dc component), the
instantaneous power signal is low-pass filtered. Figure 20
illustrates the instantaneous active power signal and shows how
the active power information can be extracted by low-pass
filtering the instantaneous power signal. This scheme correctly
calculates active power for nonsinusoidal current and voltage
waveforms at all power factors. All signal processing is carried
out in the digital domain for superior stability over temperature
and time.
Rev. A | Page 15 of 28
ADE7761
∞
∞
The low frequency output of the ADE7761 is generated by
accumulating this active power information. This low frequency
inherently means a long accumulation time between output
pulses. The output frequency is, therefore, proportional to the
average active power. This average active power information can
in turn be accumulated (for example, by a counter) to generate
active energy information. Because of its high output frequency
and therefore shorter integration time, the CF output is proportional to the instantaneous active power. This is useful for
system calibration purposes that would take place under steady
load conditions.
DIGITAL-TO-
CH1
CH2
V× I
TIME
ADC
HPF
MULTIPLIER
ADC
INSTANTANEOUS
POWER SIGNAL –p(t)
p(t) = i(t).v(t)
WHERE:
v(t) = V × cos(ϖt)
i(t) = I × cos(ϖt)
V× I
p(t) =
2
LPF
INSTANTANEOUS
ACTIVE POWER SIGNAL
V× I
{1 + cos (2ϖt)}
2
FREQUENCY
DIGITAL-TO-
FREQUENCY
F1
F2
CF
Figure 20. Signal Processing Block Diagram
Power Factor Considerations
The method used to extract the active power information from
the instantaneous power signal (by low-pass filtering) is still
valid even when the voltage and current signals are not in
phase. Figure 21 displays the unity power factor condition and
a displacement power factor (DPF = 0.5), that is, current signal
lagging the voltage by 60°. If one assumes that the voltage and
current waveforms are sinusoidal, the active power component
of the instantaneous power signal (dc term) is given by
04407-0-022
V× I
2
V× I
2
0V
× cos(60°)
0V
INSTANTANEOUS
POWER SIGNAL
CURRENT
VOLTAGE
VOLTAGE
INSTANTANEOUS
POWER SIGNAL
60°
INSTANTANEOUS
ACTIVE POWER SIGNAL
INSTANTANEOUS
ACTIVE POWER SIGNAL
CURRENT
Figure 21. Active Power Calculation over PF
Nonsinusoidal Voltage and Current
The active power calculation method also holds true for
nonsinusoidal current and voltage waveforms. All voltage and
current waveforms in practical applications have some
harmonic content. Using the Fourier transform, instantaneous
voltage and current waveforms can be expressed in terms of
their harmonic content:
)sin(2)(
thVVtvα+ω××+=
O
∑
h
0hh
≠
(1)
where:
v(t) is the instantaneous voltage.
is the average value.
V
O
is the rms value of voltage harmonic h.
V
h
is the phase angle of the voltage harmonic.
α
h
04407-0-023
(2)
)sin(2)(
(V × I/2) × cos(60°)
O
∑
h
0hh
≠
thIItiβ+ω××+=
This is the correct active power calculation.
where:
i(t) is the instantaneous current.
is the dc component.
I
O
is the rms value of current harmonic h.
I
h
is the phase angle of the current harmonic.
β
h
Rev. A | Page 16 of 28
ADE7761
Using Equations 1 and 2, the active power P can be expressed in
terms of its fundamental active power (P
power (P
):
H
PPP+=
1
H
) and harmonic active
1
where:
IVP
Φ×=)cos(
1111
β−α=Φ
111
(3)
and
∞
IVP
∑
H
h
2
=
β−α=Φ
hhh
Φ××=
)cos(
hhh
(4)
As can be seen from Equation 4, a harmonic active power
component is generated for every harmonic, provided that
harmonic is present in both the voltage and current waveforms.
The power factor calculation has previously been shown to be
accurate in the case of a pure sinusoid; the harmonic active
power must, therefore, also correctly account for power factor,
because it is made up of a series of pure sinusoids.
Note that the input bandwidth of the analog inputs is 7 kHz
with the internal oscillator frequency of 450 kHz.
HPF and Offset Effects
Equation 5 shows the effect of offsets on the active power
calculation. Figure 22 shows the effect of offsets on the active
power calculation in the frequency domain.
tItV
)()(
=×
tIItVV
))cos(())cos((
1010
IV
×
IV
+×
10
11
2
=ω×+×ω×+
0110
(5)
tIVtIV
)cos()cos(
ω××+ω××+
V1× I
1
2
Figure 22. Effect of Channel Offsets on the Active Power Calculation
0.30
0.25
0.20
0.15
0.10
0.05
PHASE (Degrees)
0
–0.05
–0.10
0100
Figure 23. Phase Error between Channels (0 Hz to 1 kHz)
0.30
0.25
0.20
0.15
0.10
DC COMPONENT (INCLUDING ERROR TERM)
IS EXTRACTED BY THE LPF FOR ACTIVE
POWER CALCULATION
V1× I
0
V0× I
1
0v
200 300 400 500 600 700 800 900 1000
FREQUENCY (RAD/S)
FREQUENCY (Hz)
2v
04407-0-024
04407-0-025
As can be seen from Equation 5 and Figure 22, an offset on
Channel 1 and Channel 2 contributes a dc component after
multiplication. Because this dc component is extracted by the
LPF and used to generate the active power information, the
offsets contribute a constant error to the active power calculation. This problem is easily avoided in the ADE7761 with the
HPF in Channel 1. By removing the offset from at least one
channel, no error component can be generated at dc by the
multiplication. Error terms at cos(ωt) are removed by the LPF
and the digital-to-frequency conversion (see the Digital-toFrequency Conversion section).
The HPF in Channel 1 has an associated phase response that is
compensated for on-chip. Figure 23 and Figure 24 show the
phase error between channels with the compensation network
activated. The ADE7761 is phase compensated up to 1 kHz as
shown, which ensures correct active harmonic power
calculation even at low power factors.
Rev. A | Page 17 of 28
0.05
PHASE (Degrees)
0
–0.05
–0.10
40
455055606570
FREQUENCY (Hz)
04407-0-026
Figure 24. Phase Error between Channels (40 Hz to 70 Hz)
ADE7761
)
V
V
×
DIGITAL-TO-FREQUENCY CONVERSION
As previously described, the digital output of the low-pass filter
after multiplication contains the active power information.
However, because this LPF is not an ideal “brick wall” filter
implementation, the output signal also contains attenuated
components at the line frequency and its harmonics, that is,
cos(hωt), where h = 1, 2, 3, …, and so on. The magnitude
response of the filter is given by
=
)(ffH
For a line frequency of 50 Hz, this gives an attenuation of the 2ω
(100 Hz) component of approximately –26.9 dB. The dominating harmonic is at twice the line frequency, cos(2ωt), due to the
instantaneous power signal.
Figure 25 shows the instantaneous active power signal output of
the LPF, which still contains a significant amount of instantaneous power information, cos(2ωt). This signal is then passed to
the digital-to-frequency converter, where it is integrated
(accumulated) over time to produce an output frequency. This
accumulation of the signal suppresses or averages out any nondc components in the instantaneous active power signal. The
average value of a sinusoidal signal is zero. Therefore, the
frequency generated by the ADE7761 is proportional to the
average active power.
Figure 25 also shows the digital-to-frequency conversion for
steady load conditions: constant voltage and current. As can be
seen in Figure 25, the frequency output CF varies over time,
even under steady load conditions. This frequency variation is
primarily due to the cos(2ωt) component in the instantaneous
active power signal.
V
MULTIPLIER
I
LPF TO EXTRACT
ACTIVE POWER
(DC TERM)
0ϖ2ϖ
FREQUENCY (Rad/s)
1
=
LPF
(6)
2
)Hz5.4/(1
F1
DIGITAL-TO-
FREQUENCY
DIGITAL-TO-
FREQUENCY
F1
F2
FOUT
CF
TIME
FREQUENCYFREQUENCY
TIME
The output frequency on CF can be up to 2048 times higher
than the frequency on F1 and F2. This higher output frequency
is generated by accumulating the instantaneous active power
signal over a much shorter time while converting it to a
frequency. This shorter accumulation period means less
averaging of the cos(2ωt) component. As a consequence, some
of this instantaneous power signal passes through the digital-tofrequency conversion. This is not a problem in the application.
Where CF is used for calibration purposes, the frequency
should be averaged by the frequency counter, which removes
any ripple. If CF is being used to measure energy, such as in a
microprocessor-based application, the CF output should also be
averaged to calculate power. Because the outputs F1 and F2
operate at a much lower frequency, a lot more averaging of the
instantaneous active power signal is carried out. The result is a
greatly attenuated sinusoidal content and a virtually ripple-free
frequency output.
TRANSFER FUNCTION
Frequency Outputs F1 and F2
The ADE7761 calculates the product of two voltage signals (on
Channel 1 and Channel 2) and then low-pass filters this product
to extract active power information. This active power information is then converted to a frequency. The frequency
information is output on F1 and F2 in the form of active high
pulses. The pulse rate at these outputs is relatively low, for
example, 0.34 Hz maximum for ac signals with S0 = S1 = 0 (see
Table 7). This means that the frequency at these outputs is
generated from active power information accumulated over a
relatively long period of time. The result is an output frequency
that is proportional to the average active power. The averaging
of the active power signal is implicit to the digital-to-frequency
conversion. The output frequency or pulse rate is related to the
input voltage signals by the following equation:
F
2170.5
××
rmsrms
−
41
FrequencyFF
1
2
=−
2
V
REF
where:
− F2 Frequency is the output frequency on F1 and F2 (Hz).
F
1
V1
is the differential rms voltage signal on Channel 1 (V).
rms
V2
is the differential rms voltage signal on Channel 2 (V).
rms
V
is the reference voltage (2.5 V ± 8%) (V).
REF
F
is one of four possible frequencies selected by using the
1–4
logic inputs S0 and S1 (see Table 5).
(7)
INSTANTANEOUS ACTIVE POWER SIGNAL (FREQUENCY DOMAIN
Values are generated using the nominal frequency of 450 kHz.
2
F
are a binary fraction of the master clock and, therefore, vary with the
1–4
internal oscillator frequency (OSC).
Frequency Output CF
The pulse output calibration frequency (CF) is intended for use
during calibration. The output pulse rate on CF can be up to
2048 times the pulse rate on F1 and F2. The lower the F
frequency selected, the higher the CF scaling. Table 6 shows
how the two frequencies are related, depending on the states of
the logic inputs S0, S1, and SCF. Because of its relatively high
pulse rate, the frequency at this logic output is proportional to
the instantaneous active power. As with F1 and F2, the
frequency is derived from the output of the low-pass filter after
multiplication. However, because the output frequency is high,
this active power information is accumulated over a much
shorter time. Therefore, less averaging is carried out in the
digital-to-frequency conversion. With much less averaging of
the active power signal, the CF output is much more responsive
to power fluctuations (see Figure 20).
Table 6. Relationship between CF and F1, F2 Frequency
Outputs
In this example, if ac voltages of ±660 mV peak are applied to
V1 and V2, then the expected output frequency on CF, F1, and
F2 is calculated as follows:
Frequency Selection
1–4
(Hz)1 OSC/CLKIN2
1–4
(Hz) CF Frequency Output
1–4
F
= 1.7 Hz, SCF = S1 = S0 = 0
1–4
= rms of 660 mV peak ac = 0.66/√2 V
V1
rms
V2
= rms of 660 mV peak ac = 0.66/√2 V
rms
1–4
Note that if the on-chip reference is used, actual output
frequencies may vary from device to device due to a reference
tolerance of ±8%.
FrequencyFF
21
=−
FFFrequencyCF
21
××
××
Hz0.2264
=×−=
Hz72.166.066.070.5
=
2
5.222
Hz34.0
As can be seen from these two example calculations, the
maximum output frequency for ac inputs is always half of that
for dc input signals. Table 7 shows a complete listing of all
maximum output frequencies for ac signals.
Table 7. Maximum Output Frequency on CF, F1, and F2 for
AC Inputs
The ADE7761 incorporates a novel fault detection scheme that
warns of fault conditions and allows the ADE7761 to continue
accurate billing during a fault event. The ADE7761 does this by
continuously monitoring both the phase and neutral (return)
currents. A fault is indicated when these currents differ by more
than 6.25%. However, even during a fault, the output pulse rate
on F1 and F2 is generated using the larger of the two currents.
Because the ADE7761 looks for a difference between the voltage
signals on V
ducers be closely matched.
On power-up, the output pulse rate of the ADE7761 is proportional to the product of the voltage signals on V
Channel 2. If there is a difference of greater than 6.25% between
V
and V1B on power-up, the fault indicator (FAULT) becomes
1A
active after about 1 s. In addition, if V
ADE7761 selects V
automatically disabled when the voltage signal on Channel 1 is
less than 0.3% of the full-scale input range. This eliminates false
detection of a fault due to noise at light loads.
and V1B, it is important that both current trans-
1A
and
1A
is greater than V1A, the
1B
as the input. The fault detection is
1B
= 2.5 V (nominal reference value)
V
REF
Rev. A | Page 19 of 28
ADE7761
C
Fault with Active Input Greater than Inactive Input
If V1A is the active current input (that is, being used for billing),
and the voltage signal on V
of V
, the fault indicator becomes active. Both analog inputs are
1A
filtered and averaged to prevent false triggering of this logic
output. As a consequence of the filtering, there is a time delay of
approximately 3 s on the logic output FAULT after the fault
event. The FAULT logic output is independent of any activity on
outputs F1 or F2. Figure 26 shows one condition under which
FAULT becomes active. Because V
still greater than V
swap to the V
V
1A
V
1B
0V
V1B < 93.75% OF V
FAULT
<0
6.25% OF ACTIVE INPUT
Figure 26. Fault Conditions for Active Input Greater than Inactive Input
, billing is maintained on V1A, that is, no
1B
input occurs. V1A remains the active input.
1B
AGND
1A
Fault with Inactive Input Greater than Active Input
Figure 27 illustrates another fault condition. If the difference
between V
, the inactive input, and V1A, the active input (that is,
1B
being used for billing), becomes greater than 6.25% of V
FAULT indicator goes active, and there is also a swap over to the
V
input. The analog input V1B becomes the active input. Again,
1B
there is a time constant of about 3 s associated with this swap.
V
does not swap back to being the active channel until V1A is
1A
greater than V
and the difference between V1A and V1B—in this
1B
order—becomes greater than 6.25% of V
FAULT indicator becomes inactive as soon as V
6.25% of V
between V
0V
. This threshold eliminates potential chatter
1B
and V1B.
1A
V
1A
V
1B
AGND
V1A < 93.75% OF V
FAULT + SWAP
1B
(inactive input) falls below 93.75%
1B
is the active input and it is
1A
V
1A
V
1A
V
1N
V
1B
V
1B
>0
ACTIVE POINT – INACTIVE INPUT
V
1A
V
1A
V
1N
V
1B
V
1B
A
B
1A
A
B
FILTER
COMPARE
. However, the
COMPARE
AND
1A
FILTER
AND
FAULT
TO
MULTIPLIER
is within
FAULT
TO
MULTIPLIER
1B
, the
04407-0-028
Calibration Concerns
Typically, when a meter is being calibrated, the voltage and
current circuits are separated as shown in Figure 28. This means
that current passes through only the phase or neutral circuit.
Figure 28 shows current being passed through the phase circuit.
This is the preferred option, because the ADE7761 starts billing
on the input V
nected to V
on power-up. The phase circuit CT is con-
1A
in the diagram. Since there is no current in the
1A
neutral circuit, the FAULT indicator comes on under these
conditions. However, this does not affect the accuracy of the
calibration and can be used as a means to test the functionality
of the fault detection.
R
F
V
1A
0V
R
F
F
R
F
C
T
TEST
URRENT
IB
IB
PHASE
240V RMS
NEUTRAL
V
AGND
RA*
RB*
VR*
*RB + VR = RF
CT
RB
RB
CT
C
Figure 28. Fault Conditions for Inactive Input Greater than Active Input
V
1A
C
F
V
1N
C
F
V
1B
V
2P
V
2N
If the neutral circuit is chosen for the current circuit in the
arrangement shown in Figure 28, this may have implications for
the calibration accuracy. The ADE7761 powers up with the V
1A
input active as normal. However, because there is no current in
the phase circuit, the signal on V
be flagged and the active input to be swapped to V
is zero. This causes a fault to
1A
(neutral).
1B
The meter can be calibrated in this mode, but the phase and
neutral CTs might differ slightly. Because under no-fault conditions all billing is carried out using the phase CT, the meter
should be calibrated using the phase circuit. Of course, both
phase and neutral circuits can be calibrated.
MISSING NEUTRAL MODE
The ADE7761 integrates a novel fault detection that warns and
allows the ADE7761 to continue to bill in case a meter is
connected to only one wire (see Figure 29). For correct
operation of the ADE7761 in this mode, the V
ADE7761 must be maintained within the specified range (5 V ±
5%). The missing neutral detection algorithm is designed to
work over a line frequency of 45 Hz to 55 Hz.
pin of the
DD
04407-0-030
<0
6.25% OF INACTIVE INPUT
>0
ACTIVE POINT – INACTIVE INPUT
04407-0-029
Figure 27. Fault Conditions for Inactive Input Greater than Active Input
Rev. A | Page 20 of 28
ADE7761
V
V
V
L
240V RMS
POWER
GENERATOR
LOAD
IB
CT
RB
RB
CT
RA*
RB*
VR*
*RB + VR = RF
C
R
F
V
R
1A
F
C
F
V1A
V
1N
0V
C
F
V
R
1B
F
F
V
2P
V
2N
C
T
04407-0-031
Figure 29. Missing Neutral System Diagram
The ADE7761 detects a missing neutral condition by continuously monitoring the voltage channel input (V
2P–V2N
). The
FAULT pin is held high when a missing neutral condition is
detected. In this mode, the ADE7761 continues to bill the
energy based on the signal level on the current channel (see
Figure 30). The billing rate or frequency outputs can be adjusted
by changing the dc level on the MISCAL pin.
1A
1N
1B
MISCA
ADC
A > B
HPF
ADC
ADC
B > A
B <> A
MISSING NEUTRAL
GAIN ADJUSMENT
ZERO
CROSSING
DETECTION
DIGITAL-
FREQUENCY
CONVERTERS
CF
Figure 30. Energy Calculation in Missing Neutral Mode
LPF
TO-
F1 F2
04407-0-032
Important Note for Billing of Active Energy
The ADE7761 provides pulse outputs—CF, F1, and F2—
intended to be used for the billing of active energy. Pulses are
generated at these outputs in two different situations.
Case 1: When the analog input V
– V2N complies with the
2P
conditions described in Figure 32, CF, F1, and F2 frequencies
are proportional to active power and can be used to bill active
energy.
Case 2: When the analog input V
– V2N does not comply with
2P
the conditions described in Figure 32, the ADE7761 does not
measure active energy, but a quantity proportional to kAh. This
quantity is used to generate pulses on the same CF, F1, and F2.
This situation is indicated when the FAULT pin is high.
Analog Devices Inc. cautions users of the ADE7761:
• Billing active energy in Case 1 is consistent with the
understanding of the quantity represented by pulses on
CF, F1, and F2 outputs (watt-hour).
• Billing active energy while the ADE7761 is in Case 2 must
be decided knowing that the entity measured by the
ADE7761 in this case is ampere-hour and not watt-hour.
Users should be aware of this limitation and decide if the
ADE7761 is appropriate for their application.
Missing Neutral Detection
The ADE7761 continuously monitors the voltage input and
detects a missing neutral condition when the voltage input peak
value is smaller than 9% of the analog full scale or when no zero
crossings are detected on this input (see Figure 31).
V
2P
FILTER AND
THRESHOLD
AGND
V2
V
2N
ADC
MISSING
NEUTRAL
|V2|
< 9% OF FULL SCALE
PEAK
V
2P–V2N
9% OF FS
0V
Figure 31. Missing Neutral Detection
Rev. A | Page 21 of 28
V2P–V
FSFS
0V
NO ZERO-CROSSING ON V2OR
2N
V2P–V
FS
0V
2N
04407-0-033
ADE7761
A
×
The ADE7761 leaves the missing neutral mode for normal
operation when both conditions are no longer valid—voltage
peak value greater than 9% of full scale and zero crossing on the
voltage channel detected (see Figure 32).
V
2P
V2
V
GND
2N
|V2|
PEAK
ZERO-CROSSING ON V2
+9% OF FS
–9% OF FS
Figure 32. Return to Normal Mode after Missing Neutral Detection
ADC
> 9% OF FULL SCALE
AND
V2P–V
2N
FS
FILTER AND
THRESHOLD
Missing Neutral Gain Calibration
When the ADE7761 is in missing neutral mode, the energy is
billed based on the active current input signal level. The
calibration of the frequency outputs in this mode can be done
with the MISCAL analog input pin. In this mode, applying a dc
voltage of 330 mV on MISCAL is equivalent to applying, in
normal mode, a pure sine wave on the voltage input with a peak
value of 330 mV. The MISCAL input can vary from 0 V to
660 mV (see the Analog Inputs section). When set to 0 V, the
frequency outputs are close to zero. When set to 660 mV dc, the
frequency outputs are twice that when MISCAL is at 330 mV
dc. In other words, Equation 7 can be used in missing neutral
mode by replacing V2
FrequencyFF
,
21
by MISCAL
rms
=
rms
√2:
rms
V
REF
MISSING
NEUTRAL
FMISCAL
2/70.5
××
41
−
2
(8)
04407-0-034
where:
F
, F2 Frequency is the output frequency on F1 and F2 (Hz).
1
V1
is the differential rms voltage signal on Channel 1 (V).
rms
MISCAL
is the differential rms voltage signal on the MISCAL
rms
pin (V).
V
is the reference voltage (2.5 V ± 8%) (V).
REF
F
is one of four possible frequencies selected by using the
1-4
logic inputs S0 and S1 (see Table 5).
Example
In normal mode, ac voltages of ±330 mV peak are applied to V1
and V2, and then the expected output frequency on F1 and F2 is
calculated as follows:
F
= 1.7 Hz, SCF = S1 = S0 = 0
1–4
V1 = rms of 330 mV peak ac = 0.33/√
V2 = rms of 330 mV peak ac = 0.33/√
V
= 2.5 V (nominal reference value)
REF
,
FrequencyFF
21
=
frequencyFFFrequencyCF
21
V
2
V
2
Hz7.133.033.070.5
××
××
5.222
=
2
=×−=
Hz084.0
Hz4.564
In missing neutral mode, ac voltage of ±330 mV peak is applied
to V1, no signal is connected on V2, and 330 mV dc input is
applied to MISCAL. With the ADE7761 in the same configuration as the previous example, the expected output frequencies
on CF, F1, and F2 are
Hz7.12/33.033.070.5
,
FrequencyFF
21
=
frequencyFFFrequencyCF
21
×
×××
2
5.22
Hz4.564,
=×=
Hz084.0
=
Rev. A | Page 22 of 28
ADE7761
*
r
e
APPLICATIONS
INTERFACING TO A MICROCONTROLLER FOR
ENERGY MEASUREMENT
The easiest way to interface the ADE7761 to a microcontroller
is to use the CF high frequency output with the output
frequency scaling set to 2048 × F1, F2. This is done by setting
SCF = 0 and S0 = S1 = 1 (see Table 7). With full-scale ac signals
on the analog inputs, the output frequency on CF is approximately 5.5 kHz. Figure 33 illustrates one scheme that could be
used to digitize the output frequency and carry out the
necessary averaging mentioned in the previous section.
CF
AVERAGE
FREQUENCY
ADE7761
CF
REVP*
FAULT**
*REVP MUST BE USED IF THE METER IS BIDIRECTIONAL OR
DIRECTION OF ENERGY FLOW IS NEEDED.
*FAULT MUST BE USED TO RECORD ENERGY IN FAULT CONDITION.
Figure 33. Interfacing the ADE7761 to an MCU
As shown, the frequency output CF is connected to an MCU
counter or port, which counts the number of pulses in a given
integration time, determined by an MCU internal timer. The
average power, proportional to the average frequency, is given
by
The energy consumed during an integration period is given by
FREQUENCY
RIPPLE
TIME
TimePowerAverageEnergy=×=×=
COUNTER
UP/DOWN
PowerActiveAverageFrequencyAverage==
Counter
Tim
MCU
LOGIC
±10%
Counter
Time
04407-0-035
CounterTime
For the purpose of calibration, this integration time could be
10 s to 20 s in order to accumulate enough pulses to ensure
correct averaging of the frequency. In normal operation, the
integration time could be reduced to 1 s or 2 s depending, for
example, on the required update rate of a display. With shorter
integration times on the MCU, the amount of energy in each
update may still have a small amount of ripple, even under
steady load conditions. However, over a minute or more, the
measured energy has no ripple.
SELECTING A FREQUENCY FOR AN ENERGY
METER APPLICATION
As shown in Table 5, the user can select one of four frequencies.
This frequency selection determines the maximum frequency
on F1 and F2. These outputs are intended to be used to drive the
energy register (electromechanical or other). Because only four
different output frequencies can be selected, the available
frequency selection has been optimized for a meter constant of
100 impulses/kWh with a maximum current of between 10 A
and 120 A. Table 8 shows the output frequency for several
maximum currents (I
cases, the meter constant is 100 impulses/kWh.
frequencies allow complete coverage of this range of
1–4
output frequencies on F1 and F2. When designing an energy
meter, the nominal design voltage on Channel 2 (voltage)
should be set to half-scale to allow for calibration of the meter
constant. The current channel should also be no more than halfscale when the meter sees maximum load, which accommodates
overcurrent signals and signals with high crest factors. Table 9
shows the output frequency on F1 and F2 when both analog
inputs are half-scale. The frequencies listed in Table 9 align well
with those listed in Table 8 for maximum load.
) with a line voltage of 240 V. In all
MAX
Rev. A | Page 23 of 28
ADE7761
Table 9. F1 and F2 Frequency with Half-Scale AC Inputs
When selecting a suitable F
frequency output at I
of 100 impulses/kWh should be compared with Column 4 of
Table 9. The frequency that is closest in Table 9 determines the
best choice of frequency (F
maximum current of 40 A is being designed, the output
frequency on F1 and F2 with a meter constant of
100 impulses/kWh is 0.266 Hz at 40 A and 240 V (from
Table 8). Looking at Table 9, the closest frequency to 0.266 Hz
in Column 4 is 0.17 Hz. Therefore, F2 (3.4 Hz; see Table 5) is
selected for this design.
Frequency Outputs
Figure 2 shows a timing diagram for the various frequency
outputs. The high frequency CF output is intended to be used
for communications and calibration purposes. CF produces a
90 ms wide, active high pulse (t
tional to active power. The CF output frequencies are given in
Table 7. As in the case of F1 and F2, if the period of CF (t
below 180 ms, the CF pulse width is set to half the period. For
example, if the CF frequency is 20 Hz, the CF pulse width is
25 ms.
1–4
Half-Scale AC Inputs (Hz)
frequency for a meter design, the
1–4
(maximum load) with a meter constant
MAX
). For example, if a meter with a
1-4
) at a frequency that is propor-
4
) falls
5
No-Load Threshold
The ADE7761 includes a no-load threshold and startup current
feature that eliminates creep effects in the meter. The ADE7761
is designed to issue a minimum output frequency. Any load
generating a frequency lower than this minimum frequency
does not cause a pulse to be issued on F1, F2, or CF. The minimum output frequency is given as 0.0045% of the full-scale
output frequency. (See Table 7 for maximum output frequencies
for ac signals).
For example, an energy meter with a meter constant of
100 impulses/kWh on F1, F2 using SCF = 1, S1 = 0, and S0 = 1,
the maximum output frequency at F1 or F2 is 0.68 Hz and 43.52
Hz on CF. The minimum output frequency at F1 or F2 is
0.0045% of 0.68 Hz or 3.06 × 10
–5
Hz. This is 1.96 × 10–3 Hz at
CF (64 × F1 Hz).
In this example, the no-load threshold is equivalent to 1.1 W of
load or a startup current of 4.6 mA at 240 V. Compare this value
to the IEC61036 specification, which states that the meter must
start up with a load equal to or less than 0.4% I
meter, 0.4% of I
is equivalent to 20 mA.
B
. For a 5 A (IB)
B
Note that the no-load threshold is not enabled when using the
high CF frequency mode: SCF = 0, S1 = S0 = 1.
NEGATIVE POWER INFORMATION
The ADE7761 detects when the current and voltage channels
have a phase shift greater than 90
wrong connection of the meter or generation of negative power.
The REVP pin output goes active high when negative power is
detected, and active low when positive power is detected. The
REVP pin output changes state as a pulse is issued on CF.
°. This mechanism can detect
Rev. A | Page 24 of 28
ADE7761
OUTLINE DIMENSIONS
7.50
7.20
6.90
2011
5.60
5.30
8.20
5.00
SEATING
PLANE
(RS-20)
0.25
0.09
7.80
7.40
8°
4°
0°
0.95
0.75
0.55
2.00 MAX
0.05 MIN
COPLANARITY
0.10
Figure 34. 20-Lead Shrink Small Outline Package [SSOP]
1
0.65
BSC
COMPLIANT TO JEDEC STANDARDS MO-150AE
1.85
1.75
1.65
0.38
0.22
10
Dimensions shown in millimeters
ORDERING GUIDE
Model Temperature Range Package Description Package Option
ADE7761ARS –40°C to +85°C Shrink Small Outline Package RS-20
ADE7761ARSRL –40°C to +85°C Shrink Small Outline Package RS-20
ADE7761ARS-REF Reference Board
Rev. A | Page 25 of 28
ADE7761
DISCLAIMER
The ADE7761 provides pulse outputs—CF, F1, and F2—
intended to be used for the billing of active energy. Pulses are
generated at these outputs in two different situations.
Case 1: When the analog input V
conditions described in Figure 32, CF, F1, and F2 frequencies
are proportional to active power and can be used to bill active
energy.
Case 2: When the analog input V
the conditions described in Figure 32, the ADE7761 does not
measure active energy, but a quantity proportional to kAh. This
quantity is used to generate pulses on the same CF, F1, and F2.
This situation is indicated when the FAULT pin is high.
– V2N complies with the
2P
– V2N does not comply with
2P
Analog Devices Inc. cautions users of the ADE7761:
• Billing active energy in Case 1 is consistent with the
understanding of the quantity represented by pulses on
CF, F1, and F2 outputs (watt-hour).
• Billing active energy while the ADE7761 is in Case 2 must
be decided knowing that the entity measured by the
ADE7761 in this case is ampere-hour and not watt-hour.
Users should be aware of this limitation and decide if the
ADE7761 is appropriate for their application.