The ALD500RAU/ALD500RA/ALD500R are integrating
dual slope analog processors, designed to operate on ±5V
power supplies for building precision analog-to-digital
converters. The ALD500RAU/ALD500RA/ALD500R
feature specifications suitable for 18 bit/17 bit/16 bit
resolution conversion, respectively. Together with three
capacitors, two resistors, and a digital controller, a precision
Analog to Digital converter with auto zero can be
implemented. The digital controller can be implemented
by an external microcontroller, under either hardware
(fixed logic) or software control. For ultra high resolution
applications, up to 23 bit conversion can be implemented
with an appropriate digital controller and software.
The ALD500R series of analog processors accept
differential inputs and the external digital controller first
counts the number of pulses at a fixed clock rate that a
capacitor requires to integrate against an unknown analog
input voltage, then counts the number of pulses required
to deintegrate the capacitor against a known internal
reference voltage. This unknown analog voltage can then
be converted by the microcontroller to a digital word, which
is translated into a high resolution number, representing
an accurate reading. This reading, when ratioed against
the reference voltage, yields an accurate, absolute voltage
measurement reading.
The ALD500R analog processors consist of on-chip digital
control circuitry to accept control inputs, integrating buffer
amplifiers, analog switches, and voltage comparators and
a highly accurate, ultra-stable voltage reference. It
functions in four operating modes, or phases, namely auto
zero, integrate, deintegrate, and integrator zero phases.
At the end of a conversion, the comparator output goes
from high to low when the integrator crosses zero during
deintegration. ALD500R analog processors also provide
direct logic interface to CMOS logic families.
GENERAL THEORY OF OPERATION
Dual-Slope Conversion Principles of Operation
The basic principle of dual-slope integrating analog to digital
converter is simple and straightforward. A capacitor, C
charged with the integrator from a starting voltage, V
INT
, for a
X
, is
fixed period of time at a rate determined by the value of an
unknown input voltage, which is the subject of measurement.
Then the capacitor is discharged at a fixed rate, based on an
external reference voltage, back to V
where the discharge
X
time, or deintegration time, is measured precisely. Both the
integration time and deintegration time are measured by a
digital counter controlled by a crystal oscillator. It can be
demonstrated that the unknown input voltage is determined
by the ratio of the deintegration time and integration time, and
is directly proportional to the magnitude of the external reference
voltage.
The major advantages of a dual-slope converter are:
a. Accuracy is not dependent on absolute values of
integration time t
and deintegration time t
INT
DINT
, but is
dependent on their relative ratios. Long-term clock frequency
variations will not affect the accuracy. A standard crystal
controlled clock running digital counters is adequate to generate
very high accuracies.
b. Accuracy is not dependent on the absolute values of
R
INT and CINT
, as long as the component values do not vary
through a conversion cycle, which typically lasts less than 1
second.
c. Offset voltage values of the analog components, such
as VX, are cancelled out and do not affect accuracy.
d. Accuracy of the system depends mainly on the accuracy
and the stability of the voltage reference value.
2Advanced Linear DevicesALD500RAU/ALD500RA/ALD500R
e. Very high resolution, high accuracy measurements
can be achieved simply and at very low cost.
An inherent benefit of the dual slope converter system is noise
immunity. The input noise spikes are integrated (averaged to
near zero) during the integration periods. Integrating ADCs
are immune to the large conversion errors that plague
successive approximation converters and other high resolution
converters and perform very well in high-noise environments.
The slow conversion speed of the integrating converter provides
inherent noise rejection with at least a 20dB/decade attenuation
rate. Interference signals with frequencies at integral multiples
of the integration period are, theoretically, completely removed.
Integrating converters often establish the integration period to
reject 50/60Hz line frequency interference signals.
The relationship of the integrate and deintegrate (charge
and discharge) of the integrating capacitor values are
shown below:
.
V
INT
= VX - (V
IN
t
/ R
. C
INT
INT
INT
)
(integrate cycle)(1)
.
= V
INT
- (V
V
X
REF
t
DINT
/ R
INT
.
C
)
INT
(deintegrate cycle)(2)
Combining equations 1 and 2 results in:
V
/ V
REF
= -t
IN
DINT
/ t
INT
(3)
V
= Reference Voltage
REF
C
= Integrating Capacitor value
INT
R
= Integrating Resistor value
INT
Actual data conversion is accomplished in two phases: Input
Signal Integration Phase and Reference Voltage Deintegration
Phase.
The integrator output is initialized to 0V prior to the start of
Input Signal Integration Phase. During Input Signal Integration
reference voltage is integrated
Phase, internal analog switches connect V
to the buffer
IN
input where it is maintained for a fixed integration time period
(t
). This fixed integration period is generally determined by
INT
a digital counter controlled by a crystal oscillator. The
application of V
a rate determined by V
polarity of V
causes the integrator output to depart 0V at
IN
.
IN
and a direction determined by the
IN
The Reference Voltage Deintegration Phase is initiated
immediately after t
, within 1 clock cycle. During
INT
ReferenceVoltage Deintegration Phase, internal analog
switches connect a reference voltage having a polarity opposite
that of V
to the integrator input. Simultaneously the same
IN
digital counter controlled by the same crystal oscillator used
above is used to start counting clock pulses. The Reference
Voltage Deintegration Phase is maintained until the comparator
output inside the dual slope analog processor changes state,
indicating the integrator has returned to 0V. At that point the
digital counter is stopped. The Deintegration time period
), as measured by the digital counter, is directly
(t
DINT
proportional to the magnitude of the applied input voltage.
where:
V
x
V
INT
V
IN
t
INT
t
DINT
= An offset voltage used as starting voltage
= Voltage change across C
during t
(equal in magnitude)
DINT
during t
INT
INT
and
= Average, or an integrated, value of input voltage
to be measured during t
(Constant VIN)
INT
= Fixed time period over which unknown voltage is
integrated
= Unknown time period over which a known
R
INT
ANALOG
INPUT
(V
)
IN
VOLTAGE
REFERENCE
OUTPUT
INTEGRATOR
t
INT
t
DINT
t
DINT
SWITCHES
S1
REF
V
IN ≈ VFULL SCALE
V
IN ≈ 1/2VFULL SCALE
V
≈
0
x
After the digital counter value has been read, the digital
counter, the integrator, and the auto zero capacitor are all
reset to zero through an Integrator Zero Phase and an Auto
Zero Phase so that the next conversion can begin again. In
practice, this process is usually automated so that analog-todigital conversion is continuously updated. The digital control
is handled by a microprocessor or a dedicated logic controller.
The output, in the form of a binary serial word, is read by a
microprocessor or a display adapter when desired.
C
INT
INTEGRATOR
-
+
SWITCH DRIVER
POLARITY CONTROL
V
INT
= 4.1V MAX
V
INT
PHASE
CONTROL
COMPARATOR
-
+
POLARITY
DETECTION
CONTROL
LOGIC
AB
MICROCONTROLLER
(CONTROL LOGIC
+ COUNTER)
C
OUT
Figure 2. Basic Dual-Slope Converter
ALD500RAU/ALD500RA/ALD500RAdvanced Linear Devices3
ABSOLUTE MAXIMUM RATINGS
Supply voltage, V
Differential input voltage range -0.3V to V+ +0.3V
Power dissipation 600 mW
Operating temperature range PE, SE package 0°C to +70°C
Operating temperature range QE package -55°C to +125°C
Storage temperature range-65°C to +150°C
Lead temperature, 10 seconds +260°C
+
13.2V
OPERATING ELECTRICAL CHARACTERISTICS
T
= 25°C V
A
+
= +5V V- = -5V (V supply ± 5V) unless otherwise specified; CAZ = C