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ADE7753ARS 数据表(PDF) 45 Page - Analog Devices |
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ADE7753ARS 数据表(HTML) 45 Page - Analog Devices |
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45 / 60 page ![]() ADE7753 Rev. C | Page 45 of 60 Calibrating Phase with an Accurate Source Example With an accurate source, line cycle accumulation is a good method of calibrating phase error. The value of LAENERGY must be obtained at two power factors, PF = 1 and PF = 0.5 inductive. SET HALF LINE CYCLES FOR ACCUMULATION IN LINECYC REGISTER ADDR. 0x1C SET ITEST = Ib, VTEST = VNOM, PF = 0.5 CALCULATE PHCAL. SEE EQUATION 59. SET MODE FOR LINE CYCLE ACCUMULATION ADDR. 0x09 = 0x0080 ENABLE LINE CYCLE ACCUMULATION INTERRUPT ADDR. 0x0A = 0x04 READ LINE ACCUMULATION ENERGY ADDR. 0x04 RESET THE INTERRUPT STATUS READ REGISTER ADDR. 0x0C INTERRUPT? NO NO YES YES RESET THE INTERRUPT STATUS READ REGISTER ADDR. 0x0C INTERRUPT? WRITE PHCAL VALUE TO THE PHCAL REGISTER: ADDR. 0x10 02875-A-011 Figure 85. Calibrating Phase with an Accurate Source For this example: Meter Constant: MeterConstant(imp/Wh) = 3.2 Line Voltage: Vnominal = 220 V Line Frequency: fl = 50 Hz CF Numerator: CFNUM = 0 CF Denominator: CFDEN = 489 Base Current: Ib = 10 A Half Line Cycles Used at Base Current: LINECYCIB = 2000 PERIOD Register: PERIOD = 8959 Expected Line Accumulation at Unity Power Factor (from Watt Gain Section: LAENERGYIB(expected) = 19186 Active Energy Reading at PF = .5 inductive: LAENERGYIB, PF = .5 = 9613 The error using Equation 56 is Error = 0021 . 0 2 19186 2 19186 9613 = − Phase Error (°) = −Arcsin ° − = ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ 07 . 0 3 0021 . 0 Using Equation 59, PHCAL is calculated to be 11. PHCAL = INT 11 13 2 0x0D 360 8959 07 . 0 = + − = + ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ ° × ° − Note that PHCAL is a signed twos complement register. The phase lead is corrected by 0.08° when the PHCAL register is set to 11: Phase Correction (°) = PERIOD PHCAL ° × − − 360 ) 0x0D ( Phase Correction (°) = ° = ° × − − 08 . 0 8960 360 ) 0x0D 11 ( VRMS and IRMS Calibration VRMS and IRMS are calculated by squaring the input in a digital multiplier. ) 2 cos( ) sin( V 2 ) sin( V 2 ) ( t V V t t t v 2 2 2 ω × − = ω × ω = (63) The square of the rms value is extracted from v2(t) by a low-pass filter. The square root of the output of this low-pass filter gives the rms value. An offset correction is provided to cancel noise and offset contributions from the input. There is ripple noise from the 2ω term because the low-pass filter does not completely attenuate the signal. This noise can be minimized by synchronizing the rms register readings with the zero crossing of the voltage signal. The IRQ output can be configured to indicate the zero crossing of the voltage signal. This flowchart demonstrates how VRMS and IRMS readings are synchronized to the zero crossings of the voltage input. SET INTERRUPT ENABLE FOR ZERO CROSSING ADDR. 0x0A = 0x0010 RESET THE INTERRUPT STATUS READ REGISTER ADDR. 0x0C INTERRUPT? NO YES 02875-A-003 READ VRMS OR IRMS ADDR. 0x17; 0x16 RESET THE INTERRUPT STATUS READ REGISTER ADDR. 0x0C Figure 86. Synchronizing VRMS and IRMS Readings with Zero Crossings |
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