ADE7754AR Analog Devices Inc, ADE7754AR Datasheet - Page 17

• Manufacturer Part Number: ADE7754AR
• Description: IC ENERY METER 3PHASE 24-SOIC
• Manufacturer: Analog Devices Inc

Specifications of ADE7754AR

• Input Impedance: 370 KOhm
• Measurement Error: 0.1%
• Voltage - I/o High: 2.4V
• Voltage - I/o Low: 0.8V
• Current - Supply: 7mA
• Voltage - Supply: 4.75 V ~ 5.25 V
• Operating Temperature: -40°C ~ 85°C
• Mounting Type: Surface Mount
• Package / Case: 24-SOIC (0.300", 7.50mm Width)
• Meter Type: 3 Phase
• For Use With: EVAL-ADE7754EBZ - BOARD EVALAUTION FOR ADE7754
• Lead Free Status / RoHS Status: Contains lead / RoHS non-compliant
• Other names: AD71049AR; AD71049AR

If the VGAIN registers are used for apparent power calibration
(WATMOD bits in VAMODE register = 1 or 2), the voltage
rms values are changed by voltage gain register value as described
in the expression
For example, when 7FFh is written to the voltage gain register,
the ADC output is scaled up by +50%. 7FFh = 2047d, 2047/
2
and ADC output is scaled by –50%. These two examples are
illustrated in Figure 21.
Voltage RMS Offset Compensation
The ADE7754 incorporates a voltage rms offset compensation
for each phase (AVRMSOS, BVRMSOS, and CVRMSOS).
These are 12-bit twos complement signed registers that can be
used to remove offsets in the voltage rms calculations. An offset
may exist in the rms calculation due to input noises and offsets
in the input samples. The offset calibration allows the contents
of the V
is applied.
n LSB of the voltage rms offset are equivalent to 64
the voltage rms register. Assuming that the maximum value from
the voltage rms calculation is 1,898,124 decimal with full-scale
ac inputs, then 1 LSB of the voltage rms offset represents 0.07%
of measurement error at –26 dB below full scale.
where V
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 then be derived
from these measurements. See the Calibration of a 3-Phase
Meter Based on the ADE7754 Application Note AN-624.
ACTIVE POWER CALCULATION
Electrical power is defined as the rate of energy flow from source
to load. It is given by the product of the voltage and current
waveforms. The resulting waveform is called the instantaneous
power signal and it is equal to the rate of energy flow at every
instant of time. The unit of power is the watt or joules/sec. Equa-
tion 5 gives an expression for the instantaneous power signal in
an ac system.
where V = rms voltage and I = rms current.
The average power over an integral number of line cycles (n) is
given by the expression in Equation 6.
REV. 0
12
= 0.5. Similarly, 800h = –2047d (signed twos complement)
Voltage rms
V
v t
i t
P
p t
p t
( )
rms
( )
( )
( )
=
rmso
RMS
= 2
= 2
nT
=
=
=
1
V
VI VI
v t
is the rms measurement without offset correction.
registers to be maintained at zero when no voltage
( )
nT
rms
∫
0
I
V
−
p t dt
0
sin(
×
( )
register
sin(
+
i t
( )
VRMSOS
cos(
ω
ω
t
=
)
t
VI
)
2ω
Phase A
t
)
×
64
=



rms
×



 
1
+
AVGAIN
2
12
n LSB of



 



(3)
(4)
(5)
(6)
–17–
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 compo-
nent of the instantaneous power signal p(t) in Equation 5 (i.e.,
VI). This is the relationship used to calculate active power in the
ADE7754 for each phase. The instantaneous power signal p(t)
is generated by multiplying the current and voltage signals in
each phase. The dc component of the instantaneous power signal
in each phase (A, B, and C) is then extracted by LPF2 (low-pass
filter) to obtain the active power information on each phase. This
process is illustrated in Figure 22. In a polyphase system, the total
electrical power is simply the sum of the real power in all active
phases. The solutions available to process the total active power
are discussed in the following section.
Since LPF2 does not have an ideal brick wall frequency
response (see Figure 23), 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.
Since the ripple is sinusoidal in nature, it is removed when the
active power signal is integrated to calculate the energy. See the
Energy Calculation section.
1A36E2Eh
D1B717h
00000h
V. I.
Figure 23. Frequency Response of the LPF Used
to Filter Instantaneous Power in Each Phase
–20
–24
–12
–16
–4
–8
0
1
INSTANTANEOUS
POWER SIGNAL
CURRENT
i(t) = 2 I sin ( t)
VOLTAGE
v(t) = 2 V sin ( t)
Figure 22. Active Power Calculation
3
FREQUENCY (Hz)
p(t) = V
10
8Hz
I – V
I cos(2 t)
30
ADE7754
ACTIVE REAL POWER
SIGNAL = V
I
100