REV. 0
–13–
ADE7751
FREQUENCY – Hz
40
PHASE – Degrees
–0.05
–0.10
0
0.05
0.10
0.15
0.20
0.25
0.30
45 50 55 60 65 70
Figure 11. Phase Error Between Channels (40 Hz to 70 Hz)
DIGITAL-TO-FREQUENCY CONVERSION
As previously described, the digital output of the low-pass filter
after multiplication contains the real power information. However,
since this LPF is not an ideal “brick wall” filter implementation,
the output signal also contains attenuated components at
the line frequency and its harmonics, i.e., cos(hωt) where
h = 1, 2, 3, . . . and so on.
The magnitude response of the filter is given by:
Hf
fHz
()
=
+
()
1
189/.
(6)
For a line frequency of 50 Hz, this would give an attenuation of
the 2 ω (100 Hz) component of approximately –22 dB. The
dominating harmonic will be at twice the line frequency, i.e.,
cos(2ωt), due to the instantaneous power signal.
Figure 12 shows the instantaneous real power signal output of LPF,
which still contains a significant amount of instantaneous power
information, i.e., cos(2ωt). This signal is then passed to the
digital-to-frequency converter where it is integrated (accumulated)
over time in order to produce an output frequency. This
accumulation of the signal will suppress or average out any
non-dc components in the instantaneous real power signal. The
average value of a sinusoidal signal is zero. Hence, the frequency
generated by the ADE7751 is proportional to the average real
power. Figure 12 shows the digital-to-frequency conversion
for steady load conditions, i.e., constant voltage and current.
As shown in the diagram, 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
real power signal. The output frequency on CF can be up to 128
times higher than the frequency on F1 and F2. This higher
output frequency is generated by accumulating the instantaneous
real power signal over a much shorter time while converting it to
a frequency. This shorter accumulation period means less aver-
aging of the cos(2ωt) component. As a consequence, some of
this instantaneous power signal passes through the digital-to-
frequency conversion. This will not be a problem in the application.
Where CF is used for calibration purposes, the frequency should
be averaged by the frequency counter. This will remove any ripple.
If CF is being used to measure energy, e.g., in a microprocessor-
based application, the CF output should also be averaged to
calculate power. However, if an energy measurement is being
made by counting pulses, no averaging is required. Because the
outputs F1 and F2 operate at a much lower frequency, a lot
more averaging of the instantaneous real power signal is carried
out. The result is a greatly attenuated sinusoidal content and a
virtually ripple-free frequency output.
2
V I
2
FREQUENCY – RAD/S
LPF
DIGITAL-TO-
FREQUENCY
F1
F2
DIGITAL-TO-
FREQUENCY
CF
INSTANTANEOUS REAL POWER SIGNAL
(FREQUENCY DOMAIN)
MULTIPLIER
TIME
FREQUENCY
F1
FREQUENCY
CF
TIME
V
I
0
LPF TO EXTRACT
REAL POWER
(DC TERM)
cos(2t)
ATTENUATED BY LPF
Figure 12. Real Power-to-Frequency Conversion
FAULT DETECTION
The ADE7751 incorporates a novel fault detection scheme that
warns of fault conditions and allows the ADE7751 to continue
accurate billing during a fault event. The fault detection function is
designed to work over a line frequency of 45 Hz to 55 Hz. The
ADE7751 does this by continuously monitoring both the phase
and neutral (return) currents. A fault is indicated when these
currents differ by more than 12.5%. However, even during a
fault, the output pulse rate on F1 and F2 is generated using the
larger of the two currents. Because the ADE7751 looks for a
difference between the signals on V1A and V1B, it is important
that both current transducers are closely matched.
On power-up the output pulse rate of the ADE7751 is proportional
to the product of the signals on Channel V1A and Channel 2. If
there is a difference of greater than 12.5% between V1A and
V1B on power-up, the fault indicator (FAULT) will go active
after about one second. In addition, if V1B is greater than V1A
the ADE7751 will select V1B as the input. The fault detection is
automatically disabled when the voltage signal on Channel 1 is less
than 0.5% of the full-scale input range. This will eliminate false
detection of a fault due to noise at light loads.
Fault with Active Input Greater than Inactive Input
If V1A is the active current input (i.e., is being used for billing),
and the signal on V1B (inactive input) falls by more than 12.5%
of V1A, the fault indicator will go active. Both analog inputs are
filtered and averaged to prevent false triggering of this logic
output. As a consequence of the filtering, there is a time delay of
approximately one second on the logic output FAULT after the
fault event. The FAULT logic output is independent of any activ-
ity on outputs F1 or F2. Figure 13 illustrates one condition under
which FAULT becomes active. Since V1A is the active input and it
is still greater than V1B, billing is maintained on VIA, i.e., no swap
to the V1B input will occur. V1A remains the active input.
REV. 0
ADE7751
–14–
V1B < 87.5% OF V1A
0V
V1A
V1B
V1A
V1A
V1N
AGND
V1B
V1B
FILTER
AND
COMPARE
TO
MULTIPLIER
FAULT
A
B
Figure 13. Fault Conditions for Inactive Input
Less than Active Input
Fault with V1B Greater than V1A
Figure 14 illustrates another fault condition. If V1A is the active
input (i.e., is being used for billing) and the voltage signal on
V1B (inactive input) becomes greater than 114% of V1A, the
FAULT indicator goes active, and there is also a swap over to
the V1B input. The analog input V1B has now become the
active input. Again there is a time delay of about 1.2 seconds
associated with this swap. V1A will not swap back to being the
active channel until V1A becomes greater than 114% of V1B.
However, the FAULT indicator will become inactive as soon as
V1A is within 12.5% of V1B. This threshold eliminates poten-
tial chatter between V1A and V1B.
V1A < 87.5% OF V1B
OR
V1B > 114% OF V1A
0V
V1A
V1B
V1A
V1A
V1N
AGND
V1B
V1B
FILTER
AND
COMPARE
TO
MULTIPLIER
FAULT
A
B
Figure 14. Fault Conditions for Inactive Input
Greater than Active Input
Calibration Concerns
Typically, when a meter is being calibrated, the voltage and current
circuits are separated as shown in Figure 15. This means that
current will only pass through the phase or neutral circuit. Figure 15
shows current being passed through the phase circuit. This is the
preferred option since the ADE7751 starts billing on the input
V1A on power-up. The phase circuit CT is connected to V1A in
the diagram. Since there is no current in the neutral circuit, the
FAULT indicator will come 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.
If the neutral circuit is chosen for the current circuit in the
arrangement shown in Figure 15, it may have implications for
the calibration accuracy. The ADE7751 will power up with the
V1A input active as normal. However, since there is no current
in the phase circuit, the signal on V1A is zero. This will cause a
FAULT to be flagged and the active input to be swapped to V1B
(Neutral). The meter may be calibrated in this mode, but the
phase and neutral CTs may differ slightly. Since 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 may be calibrated.
Ib
V
240Vrms
NOTE
Ra
R
f
;
Rb + VR = R
f
Rb
Rb
V1A
0V
V1B
CT
V1A
AGND
R
f
CT
NEUTRAL
PHASE
V1N
C
f
C
f
R
f
Rb
VR
V2P
R
f
V2N
C
f
C
f
TEST
CURRENT
Ib
Ra
Figure 15. Fault Conditions for Inactive
Input Greater than Active Input
TRANSFER FUNCTION
Frequency Outputs F1 and F2
The ADE7751 calculates the product of two voltage signals (on
Channel 1 and Channel 2) and then low-pass filters this product
to extract real power information. This real power information
is then converted to a frequency. The frequency information is
output on F1 and F2 in the form of active low pulses. The pulse
rate at these outputs is relatively low, e.g., 0.34 Hz maximum for
ac signals with S0 = S1 = 0 (see Table III). This means that the
frequency at these outputs is generated from real power informa-
tion accumulated over a relatively long period of time. The result is
an output frequency that is proportional to the average real
power. The averaging of the real 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.
Freq
VV Gain F
V
REF
=
×× × ×574 1 2
14
2
.
(7)
where,
Freq =Output frequency on F1 and F2 (Hz)
V1=Differential rms voltage signal on Channel 1 (Volts)
V2=Differential rms voltage signal on Channel 2 (Volts)
Gain = 1, 2, 8, or 16, depending on the PGA gain selection
made using logic inputs G0 and G1
V
REF
=The reference voltage (2.5 V ± 8%) (Volts)
F
1–4
=One of four possible frequencies selected by using the
logic inputs S0 and S1 (see Table II)
Table II.
S1 S0 F
1–4
(Hz) XTAL/CLKIN*
00 1.7 3.579 MHz/2
21
01 3.4 3.579 MHz/2
20
10 6.8 3.579 MHz/2
19
11 13.6 3.579 MHz/2
18
*F
1–4
are a binary fraction of the master clock and will thus vary if the specified
CLKIN frequency is altered.
REV. 0
ADE7751
–15–
Table IV.
F
1–4
CF Max for AC Signals
SCF S1 S0 (Hz) (Hz)
1001.7 128 × F1, F2 = 43.52
0001.7 64 × F1, F2 = 21.76
1013.4 64 × F1, F2 = 43.52
0013.4 32 × F1, F2 = 21.76
1106.8 32 × F1, F2 = 43.52
0106.8 16 × F1, F2 = 21.76
11113.6 16 × F1, F2 = 43.52
01113.6 8 × F1, F2 = 21.76
SELECTING A FREQUENCY FOR AN ENERGY METER
APPLICATION
As shown in Table II, 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). Since only four
different output frequencies can be selected, the available
frequency selection has been optimized for a meter constant of
100 imp/kWhr with a maximum current of between 10 A and
120 A. Table V shows the output frequency for several maximum
currents (I
MAX
) with a line voltage of 220 V. In all cases, the
meter constant is 100 imp/kWhr.
Table V.
I
MAX
F1 and F2 (Hz)
12.5 A 0.076
25 A 0.153
40 A 0.244
60 A 0.367
80 A 0.489
120 A 0.733
The F
1–4
frequencies allow complete coverage of this range of
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 half scale when the
meter sees maximum load. This will allow overcurrent signals and
signals with high crest factors to be accommodated. Table VI
shows the output frequency on F1 and F2 when both analog
inputs are half scale. The frequencies listed in Table VI align very
well with those listed in Table V for maximum load.
Table VI.
Frequency on F1 and F2 –
CH1 and CH2
S1 S0 F
1–4
Half-Scale AC Inputs
00 1.7 0.085 Hz
01 3.4 0.17 Hz
10 6.8 0.34 Hz
11 13.6 0.68 Hz
Example 1
If full-scale differential dc voltages of +660 mV and –660 mV are
applied to V1 and V2 respectively (660 mV is the maximum
differential voltage that can be connected to Channel 1 and
Channel 2), the expected output frequency is calculated as follows.
Gain = 1, G0 = G1 = 0
F
1–4
= 1.7 Hz, S0 = S1 = 0
V1 = +660 mV dc = 0.66 V (rms of dc = dc)
V2 = –660 mV dc = 0.66 V (rms of dc = |dc|)
V
REF
= 2.5 V (nominal reference value)
Note: If the on-chip reference is used, actual output frequencies
may vary from device to device due to reference tolerance of ±8%.
Freq
Hz
Hz=
××××
=
574 066 066 1 17
25
068
2
... .
.
.
(8)
Example 2
In this example, if ac voltages of ±660 mV peak are applied to
V1 and V2, the expected output frequency is calculated as follows.
Gain = 1, G0 = G1 = 0
F
1–4
= 1.7 Hz, S0 = S1 = 0
V1 = rms of 660 mV peak ac = 0.66/2 V
V2 = rms of 660 mV peak ac = 0.66/2 V
V
REF
= 2.5 V (nominal reference value)
Note: If the on-chip reference is used, actual output frequencies
may vary from device to device due to reference tolerance of ±8%.
Freq
Hz
Hz=
××××
××
=
574 066 066 1 17
2225
034
2
... .
.
.
(9)
As shown in these two example calculations, the maximum
output frequency for ac inputs is always half of that for dc
input signals. Table III shows a complete listing of all maxi-
mum output frequencies.
Table III.
Max Frequency Max Frequency
S1 S0 for DC Inputs (Hz) for AC Inputs (Hz)
00 0.68 0.34
01 1.36 0.68
10 2.72 1.36
11 5.44 2.72
Frequency Output CF
The pulse output CF (calibration frequency) is intended for use
during calibration. The output pulse rate on CF can be up to 128
times the pulse rate on F1 and F2. The lower the F
1–4
frequency
selected the higher the CF scaling. Table IV 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
real power. As is the case 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 real power information
is accumulated over a much shorter time. Hence, less averaging
is carried out in the digital-to-frequency conversion. With much
less averaging of the real power signal, the CF output is much
more responsive to power fluctuations (see Figure 2).

ADE7751ARSZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Data Acquisition ADCs/DACs - Specialized SGL Phase Energy Metering IC
Lifecycle:
New from this manufacturer.
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