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ADE7569 Datasheet(PDF) 62 Page - Analog Devices |
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ADE7569 Datasheet(HTML) 62 Page - Analog Devices |
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62 / 152 page ![]() ADE7116/ADE7156/ADE7166/ADE7169/ADE7566/ADE7569 Rev. B | Page 62 of 152 Voltage Channel RMS Calculation Figure 63 shows details of the signal processing chain for the rms calculation on the voltage channel. This voltage rms estimation is done in the ADE7116/ADE7156/ADE7166/ADE7169/ ADE7566/ADE7569 using the mean absolute value calculation, as shown in Figure 63. The voltage channel rms value is processed from the samples used in the voltage channel waveform sampling mode and is stored in the unsigned 24-bit Vrms register. The update rate of the voltage channel rms measurement is MCLK/5. To minimize noise in the reading of the register, the Vrms register can also be configured to update only with the zero crossing of the voltage input. This configuration is done by setting the ZXRMS bit (Bit 2) in the MODE2 register (Address 0x0C). With the specified full-scale ac analog input signal of 0.4 V, the output from LPF1 in Figure 63 swings between 0x28F5 and 0xD70B at 60 Hz (see the Voltage Channel ADC section). The equivalent rms value of this full-scale ac signal is approximately 0d1,898,124 (0x1CF68C) in the Vrms register. The voltage rms measurement provided in the ADE7116/ADE7156/ADE7166/ ADE7169/ADE7566/ADE7569 is accurate to within ±0.5% for signal input between full scale and full scale/20. The conversion from the register value to volts must be done externally in the microprocessor using a V/LSB constant. Voltage Channel RMS Offset Compensation The ADE7116/ADE7156/ADE7166/ADE7169/ADE7566/ ADE7569 incorporate a voltage channel rms offset compensation register (VRMSOS). This is a 12-bit signed register that can be used to remove offset in the voltage channel rms calculation. An offset can exist in the rms calculation due to input noises and dc offset in the input samples. One LSB of the voltage channel rms offset is equivalent to 64 LSBs of the rms register. Assuming that the maximum value from the voltage channel rms calculation is 0d1,898,124 with full-scale ac inputs, then 1 LSB of the voltage channel rms offset represents 3.37% of measurement error at −60 dB down from full scale. Vrms = Vrms0 + 64 × VRMSOS (7) where Vrms0 is the rms measurement without offset correction. ACTIVE POWER CALCULATION Active power is defined as the rate of energy flow from source to load. It is the product of the voltage and current waveforms. The resulting waveform is called the instantaneous power signal and is equal to the rate of energy flow at every instant of time. The unit of power is the watt or joules/second. Equation 8 gives an expression for the instantaneous power signal in an ac system. () ) sin( 2 t V t v ω × = (8) () ) sin( 2 t I t i ω × = (9) where: v is the rms voltage. i is the rms current. ) ( ) ( ) ( t i t v t p × = ) 2 cos( ) ( t VI VI t p ω − = (10) The average power over an integral number of line cycles (n) is given by the expression in Equation 11. ∫ = = nT VI dt t p nT P 0 ) ( 1 (11) 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 component of the instantaneous power signal p(t) in Equation 11, that is, VI. This is the relationship used to calculate active power in the ADE7116/ ADE7156/ADE7166/ADE7169/ADE7566/ADE7569. The instan- taneous power signal p(t) is generated by multiplying the current and voltage signals. The dc component of the instantaneous power signal is then extracted by LPF2 (low-pass filter) to obtain the active power information. This process is illustrated in Figure 64. INSTANTANEOUS POWER SIGNAL p(t) = v × i – v × i × cos(2ωt) ACTIVE REAL POWER SIGNAL = v × i 0x19999A VI 0xCCCCD 0x00000 CURRENT i(t) = √2 × i × sin(ωt) VOLTAGE v(t) = √2 × v × sin(ωt) Figure 64. Active Power Calculation Because LPF2 does not have an ideal brick wall frequency response (see Figure 65), 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. Because of its sinusoidal nature, the ripple is removed when the active power signal is integrated to calculate energy (see the Active Energy Calculation section). |
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