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ADE7761AARS-REF 数据表(PDF) 14 Page - Analog Devices |
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ADE7761AARS-REF 数据表(HTML) 14 Page - Analog Devices |
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14 / 24 page ![]() ADE7761A Rev. 0 | Page 14 of 24 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 22 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. F2 CF F1 DIGITAL-TO- FREQUENCY DIGITAL-TO- FREQUENCY HPF MULTIPLIER LPF ADC ADC CH1 CH2 INSTANTANEOUS POWER SIGNAL –p(t) INSTANTANEOUS ACTIVE POWER SIGNAL V × I V × I 2 TIME p(t) = i(t).v(t) WHERE: v(t) = V × cos(ωt) i(t) = I × cos(ωt) p(t) = V × I {1 + cos (2ωt)} 2 PGA Figure 22. Signal Processing Block Diagram The low frequency output of the ADE7761A 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 take place under steady load conditions. 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 23 displays the unity power factor condition and a displacement power factor (DPF = 0.5), that is, current signal lagging the voltage by 60°. INSTANTANEOUS POWER SIGNAL INSTANTANEOUS ACTIVE POWER SIGNAL INSTANTANEOUS POWER SIGNAL INSTANTANEOUS ACTIVE POWER SIGNAL 60° CURRENT CURRENT VOLTAGE 0V 0V VOLTAGE V × I 2 V × I 2 × cos(60°) Figure 23. Active Power Calculation over PF 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 (V × I/2) × cos(60°) This is the correct active power calculation. 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 ) ( 0 h h h O t h V V t v α + ω × × + = ∑ ∞ ≠ (1) where: v(t) is the instantaneous voltage. VO is the average value. Vh is the rms value of voltage harmonic h. αh is the phase angle of the voltage harmonic. |
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