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MCP3906AT-I/SS Datasheet(PDF) 18 Page - Microchip Technology |
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MCP3906AT-I/SS Datasheet(HTML) 18 Page - Microchip Technology |
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18 / 32 page ![]() MCP3905A/05L/06A DS22011B-page 18 © 2006-2011 Microchip Technology Inc. The multiplier output gives the product of the two high- pass filtered channels, corresponding to instantaneous real power. Multiplying two sine wave signals by the same ω frequency gives a DC component and a 2ω component. The instantaneous power signal contains the real power of its DC component, while also contain- ing 2 ω components coming from the line frequency multiplication. These 2 ω components come for the line frequency (and its harmonics) and must be removed in order to extract the real-power information. This is accomplished using the low-pass filter and DTF converter. 4.6 Low-Pass Filter and DTF Converter The MCP3905A/05L/06A low-pass filter is a first-order IIR filter that extracts the active real-power information (DC component) from the instantaneous power signal. The magnitude response of this filter is detailed in Figure 4-5. Due to the fact that the instantaneous power signal has harmonic content (coming from the 2 ω components of the inputs), and since the filter is not ideal, there will be some ripple at the output of the low- pass filter at the harmonics of the line frequency. The cut-off frequency of the filter (8.9 Hz) has been chosen to have sufficient rejection for commonly-used line frequencies (50 Hz and 60 Hz). With a standard input clock (MCLK = 3.58 MHz) and a 50 Hz line frequency, the rejection of the 2 ω component (100 Hz) will be more than 20 dB. This equates to a 2 ω component containing 10 times less power than the main DC component (i.e., the average active real power). FIGURE 4-5: LPF Magnitude Response (MCLK = 3.58 MHz). The output of the low-pass filter is accumulated in the digital-to-frequency converter. This accumulation is compared to a different digital threshold for FOUT0/1 and HFOUT, representing a quantity of real energy mea- sured by the part. Every time the digital threshold on FOUT0/1 or HFOUT is crossed, the part will output a pulse (See Section 4.7 “FOUT0/1 and HFOUT Output Frequencies”). The equivalent quantity of real energy required to output a pulse is much larger for the FOUT0/1 outputs than the HFOUT. This is such that the integration period for the FOUT0/1 outputs is much larger. This larger integration period acts as another low-pass filter so that the output ripple due to the 2 ω components is minimal. However, these components are not totally removed, since realized low-pass filters are never ideal. This will create a small jitter in the output frequency. Averaging the output pulses with a counter or a MCU in the application will then remove the small sinusoidal content of the output frequency and filter out the remaining 2 ω ripple. HFOUT is intended to be used for calibration purposes due to its instantaneous power content. The shorter integration period of HFOUT demands that the 2ω component be given more attention. Since a sinusoidal signal average is zero, averaging the HFOUT signal in steady-state conditions will give the proper real energy value. 4.7 FOUT0/1 and HFOUT Output Frequencies The thresholds for the accumulated energy are different for FOUT0/1 and HFOUT (i.e., they have different transfer functions). The FOUT0/1 allowed output frequencies are quite low in order to allow superior integration time (see Section 4.6 “Low-Pass Filter and DTF Converter”). The FOUT0/1 output frequency can be calculated with the following equation: EQUATION 4-1: FOUT FREQUENCY OUTPUT EQUATION For a given DC input V, the DC and RMS values are equivalent. For a given AC input signal with peak-to- peak amplitude of V, the equivalent RMS value is V/sqrt(2), assuming purely sinusoidal signals. Note that since the real power is the product of two RMS inputs, the output frequencies of AC signals are half of the DC inputs ones, again assuming purely sinusoidal AC signals. The constant FC depends on the FOUT0 and FOUT1 digital settings. Table 4-3 shows FOUT0/1 output frequencies for the different logic settings. -40 -35 -30 -25 -20 -15 -10 -5 0 0.1 1 10 100 1000 Frequency (Hz) F OUT Hz () 8.06 V 0 × V 1 × GF C × × V REF ()2 ----------------------------------------------------------- = Where: V0 is the RMS differential voltage on Channel 0 V1 is the RMS differential voltage on Channel 1 G is the PGA gain on Channel 0 (current channel) FC is the frequency constant selected VREF is the voltage reference |
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