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ADE7753ARSZ 数据表(PDF) 31 Page - Analog Devices |
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ADE7753ARSZ 数据表(HTML) 31 Page - Analog Devices |
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31 / 60 page ![]() ADE7753 Rev. C | Page 31 of 60 0xFFFF,FFFF,FFFF before it overflows. The integration time under these conditions with WDIV = 0 is calculated as follows: Time = xCCCCD 0 FFFF FFFF, xFFFF, 0 × 1.12 μs = 375.8 s = 6.26 min(15) When WDIV is set to a value different from 0, the integration time varies, as shown in Equation 16. WDIV Time Time WDIV × = =0 (16) POWER OFFSET CALIBRATION The ADE7753 also incorporates an active power offset register (APOS[15:0]). This is a signed twos complement 16-bit register that can be used to remove offsets in the active power calculation— see Figure 65. An offset could exist in the power calculation due to crosstalk between channels on the PCB or in the IC itself. The offset calibration allows the contents of the active power register to be maintained at 0 when no power is being consumed. The 256 LSBs (APOS = 0x0100) written to the active power offset register are equivalent to 1 LSB in the waveform sample register. Assuming the average value, output from LPF2 is 0xCCCCD (838,861d) when inputs on Channels 1 and 2 are both at full scale. At −60 dB down on Channel 1 (1/1000 of the Channel 1 full-scale input), the average word value output from LPF2 is 838.861 (838,861/1,000). One LSB in the LPF2 output has a measurement error of 1/838.861 × 100% = 0.119% of the average value. The active power offset register has a resolution equal to 1/256 LSB of the waveform register, therefore the power offset correction resolution is 0.00047%/LSB (0.119%/256) at –60 dB. ENERGY-TO-FREQUENCY CONVERSION ADE7753 also provides energy-to-frequency conversion for calibration purposes. After initial calibration at manufacturing, the manufacturer or end customer often verify the energy meter calibration. One convenient way to verify the meter calibration is for the manufacturer to provide an output frequency, which is proportional to the energy or active power under steady load conditions. This output frequency can provide a simple, single- wire, optically isolated interface to external calibration equipment. Figure 67 illustrates the energy-to-frequency conversion in the ADE7753. CFNUM[11:0] CF 11 0 CFDEN[11:0] 11 0 AENERGY[48:0] 48 0 02875-0-066 % DFC Figure 67. ADE7753 Energy-to-Frequency Conversion A digital-to-frequency converter (DFC) is used to generate the CF pulsed output. The DFC generates a pulse each time 1 LSB in the active energy register is accumulated. An output pulse is generated when (CFDEN + 1)/(CFNUM + 1) number of pulses are generated at the DFC output. Under steady load conditions, the output frequency is proportional to the active power. The maximum output frequency, with ac input signals at full scale and CFNUM = 0x00 and CFDEN = 0x00, is approximately 23 kHz. The ADE7753 incorporates two registers, CFNUM[11:0] and CFDEN[11:0], to set the CF frequency. These are unsigned 12-bit registers, which can be used to adjust the CF frequency to a wide range of values. These frequency-scaling registers are 12-bit registers, which can scale the output frequency by 1/212 to 1 with a step of 1/212. If the value 0 is written to any of these registers, the value 1 would be applied to the register. The ratio (CFNUM + 1)/ (CFDEN + 1) should be smaller than 1 to ensure proper operation. If the ratio of the registers (CFNUM + 1)/(CFDEN + 1) is greater than 1, the register values would be adjusted to a ratio (CFNUM + 1)/(CFDEN + 1) of 1. For example, if the output frequency is 1.562 kHz while the contents of CFDEN are 0 (0x000), then the output frequency can be set to 6.1 Hz by writing 0xFF to the CFDEN register. When CFNUM and CFDEN are both set to one, the CF pulse width is fixed at 16 CLKIN/4 clock cycles, approximately 18 μs with a CLKIN of 3.579545 MHz. If the CF pulse output is longer than 180 ms for an active energy frequency of less than 5.56 Hz, the pulse width is fixed at 90 ms. Otherwise, the pulse width is 50% of the duty cycle. The output frequency has a slight ripple at a frequency equal to twice the line frequency. This is due to imperfect filtering of the instantaneous power signal to generate the active power signal— see the Active Power Calculation section. Equation 9 from the Active Power Calculation section gives an expression for the instantaneous power signal. This is filtered by LPF2, which has a magnitude response given by Equation 17. 2 9 . 8 1 1 ) ( 2 f f H + = (17) The active power signal (output of LPF2) can be rewritten as p(t) = VI − ⎥ ⎥ ⎥ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣ ⎡ ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + 2 9 . 8 1 L 2f VI × cos(4πfLt) (18) where fL is the line frequency, for example, 60 Hz. From Equation 13, E(t) = VIt − ⎥ ⎥ ⎥ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣ ⎡ ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + π 2 9 . 8 1 4 L L 2f f VI × sin(4πfLt) (19) |
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