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参数资料
| 型号： | ADE7751ARSZ |
| 厂商： | Analog Devices Inc |
| 文件页数： | 15/16页 |
| 文件大小： | 0K |
| 描述： | IC ENERGY METERING 1PHASE 24SSOP |
| 标准包装： | 59 |
| 输入阻抗： | 390 千欧 |
| 测量误差： | 0.1% |
| 电压 - 高输入/输出： | 2.4V |
| 电压 - 低输入/输出： | 0.8V |
| 电流 - 电源： | 3mA |
| 电源电压： | 4.75 V ~ 5.25 V |
| 测量仪表类型： | 单相 |
| 工作温度： | -40°C ~ 85°C |
| 安装类型： | 表面贴装 |
| 封装/外壳： | 24-SSOP（0.209"，5.30mm 宽） |
| 供应商设备封装： | 24-SSOP |
| 包装： | 管件 |
| 配用： | EVAL-ADE7751ZEB-ND - BOARD EVALUATION FOR ADE7751 |
ADE7751
Example 1
Table IV.
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%.
SCF
1
0
1
0
1
0
1
0
S1
0
0
0
0
1
1
1
1
S0
0
0
1
1
0
0
1
1
F 1–4
(Hz)
1.7
1.7
3.4
3.4
6.8
6.8
13.6
13.6
CF Max for AC Signals
(Hz)
128 × F1, F2 = 43.52
64 × F1, F2 = 21.76
64 × F1, F2 = 43.52
32 × F1, F2 = 21.76
32 × F1, F2 = 43.52
16 × F1, F2 = 21.76
16 × F1, F2 = 43.52
8 × F1, F2 = 21.76
Freq =
5.74 × 0.66 × 0.66 × 1 × 1.7 Hz
2 . 5 2
= 0 . 68 Hz
(8)
SELECTING A FREQUENCY FOR AN ENERGY METER
APPLICATION
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
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
F 1–4
V1
V2
V REF
=
=
=
=
1.7 Hz, S0 = S1 = 0
rms of 660 mV peak ac = 0.66/ √ 2 V
rms of 660 mV peak ac = 0.66/ √ 2 V
2.5 V (nominal reference value)
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
Note: If the on-chip reference is used, actual output frequencies
may vary from device to device due to reference tolerance of ± 8%.
meter constant is 100 imp/kWhr.
Table V.
Freq =
5.74 × 0.66 × 0.66 × 1 × 1.7 Hz
2 × 2 × 2 . 5 2
= 0 . 34 Hz
(9)
I MAX
12.5 A
F1 and F2 (Hz)
0.076
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.
25 A
40 A
60 A
80 A
120 A
0.153
0.244
0.367
0.489
0.733
Table III.
The F 1–4 frequencies allow complete coverage of this range of
S1
0
0
1
1
S0
0
1
0
1
Max Frequency
for DC Inputs (Hz)
0.68
1.36
2.72
5.44
Max Frequency
for AC Inputs (Hz)
0.34
0.68
1.36
2.72
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
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
well with those listed in Table V for maximum load.
Table VI.
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
S1
0
0
1
1
S0
0
1
0
1
F 1–4
1.7
3.4
6.8
13.6
Frequency on F1 and F2 –
CH1 and CH2
Half-Scale AC Inputs
0.085 Hz
0.17 Hz
0.34 Hz
0.68 Hz
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).
REV. 0
–15 –
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