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ADE7758ARWRL 数据表(PDF) 36 Page - Analog Devices |
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ADE7758ARWRL 数据表(HTML) 36 Page - Analog Devices |
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36 / 68 page ![]() ADE7758 Rev. A | Page 36 of 68 to twice the line frequency. Because the ripple is sinusoidal in nature, it is removed when the reactive power signal is integrated over time to calculate the reactive energy. The phase-shift filter has –90° phase shift when the integrator is enabled and +90° phase shift when the integrator is disabled. In addition, the filter has a nonunity magnitude response. Because the phase-shift filter has a large attenuation at high frequency, the reactive power is primarily for the calculation at line frequency. The effect of harmonics is largely ignored in the reactive power calculation. Note that because of the magnitude characteristic of the phase shifting filter, the LSB weight of the reactive power calculation is slightly different from that of the active power calculation (see the Energy Registers Scaling section). Reactive Power Gain Calibration The average reactive power from the LPF output in each phase can be scaled by ±50% by writing to the phase’s VAR gain register (AVARG, BVARG, or CVARG). The VAR gain registers are twos complement, signed registers, and have a resolution of 0.024%/LSB. The function of the VAR gain registers is expressed below. = Power Reactive Average ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + × 12 2 1 Register Gain VAR Output LPF2 The output is scaled by –50% when the VAR gain registers contents are set to 0x800 and the output is increased by +50% by writing 0x7FF to the VAR gain register. This register can be used to calibrate the reactive power (or energy) calculation in the ADE7758 for each phase. Reactive Power Offset Calibration The ADE7758 incorporates a VAR offset register on each phase (AVAROS, BVAROS, and CVAROS). These are signed twos complement, 12-bit registers that are used to remove offsets in the reactive power calculations. An offset may exist in the power calculation due to crosstalk between channels on the PCB or in the chip itself. The offset calibration allows the contents of the reactive power register to be maintained at 0 when no reactive power is being consumed. The offset registers’ resolution is the same as the active power offset registers (see the Apparent Power Offset Calibration section). Sign of Reactive Power Calculation Note that the average reactive power is a signed calculation. As stated previously, the phase shift filter has –90° phase shift when the integrator is enabled and +90° phase shift when the integrator is disabled. Table 8 summarizes the relationship between the phase difference between the voltage and the current and the sign of the resulting VAR calculation. The ADE7758 has a sign detection circuit for the reactive power calculation. The REVPRP bit (Bit 18) in the interrupt status register is set if the average reactive power from any one of the phases changes. The phases monitored are selected by TERMSEL bits in the COMPMODE register (see Table 17). If the REVPRP bit is set in the mask register, the IRQ logic output goes active low (see the ADE7758 Interrupts section). Note that this bit is set whenever there is a sign change, i.e., the bit is set for both a positive-to-negative change or a negative-to-positive change of the sign bit. Table 8. Sign of Reactive Power Calculation Φ1 Integrator Sign of Reactive Power Between 0 to +90 Off Positive Between −90 to 0 Off Negative Between 0 to +90 On Positive Between −90 to 0 On Negative ____________________________________________________ 1 Φ is defined as the phase angle of the voltage signal minus the current signal, i.e., Φ is positive if the load is inductive and negative if the load is capacitive. Reactive Energy Calculation Reactive energy is defined as the integral of reactive power. ()dt t q Energy Reactive ∫ = (19) Similar to active power, the ADE7758 achieves the integration of the reactive power signal by continuously accumulating the reactive power signal in the internal 41-bit accumulation registers. The VAR-hr registers (AVARHR, BVARHR, and CVARHR) represent the upper 16 bits of these internal registers. This discrete time accumulation or summation is equivalent to integration in continuous time. Equation 20 expresses the relationship () () ⎭ ⎬ ⎫ ⎩ ⎨ ⎧ × = = ∑ ∫ ∞ = → 0 n T T nT q Lim dt t q Energy Reactive 0 (20) where n is the discrete time sample number and T is the sample period. Figure 72 shows the signal path of the reactive energy accumula- tion. The average reactive power signal is continuously added to the internal reactive energy register. This addition is a signed operation. Negative energy is subtracted from the reactive energy register. The average reactive power is divided by the content of the VAR divider register before they are added to the corre- sponding VAR-hr accumulation registers. When the value in the VARDIV[7:0] register is 0 or 1, the reactive power is accumulated without any division. VARDIV is an 8-bit unsigned register that is useful to lengthen the time it takes before the VAR-hr accumulation registers overflow. Similar to reactive power, the fastest integration time occurs when the VAR gain registers are set to maximum full scale, i.e., 0x7FF. The time it takes before overflow can be scaled by writing to the VARDIV register and therefore it can be increased by a maximum factor of 255. |
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