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PM4104APDA Datasheet(PDF) 4 Page - Sames |
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PM4104APDA Datasheet(HTML) 4 Page - Sames |
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4 / 14 page ![]() http://www.sames.co.za 4/14 PRELIMINARY PM4104APDA Current Input Filtering For best immunity to electromagnetic disturbances the SA4104A/B requires low-pass filters on the current sense inputs. Referring to Figure 2 and Figure 3, these filters are realized by means of the capacitors C1 and C2. The typical cut-off frequency of these filters should be between 10kHz and 20kHz. The equivalent resistance associated with each capacitor is RC/2 so the capacitor value should be in the order of C C CI C R f 1 C2 C1 = p = = where fCI is the required cut-off frequency of the low-pass filters of the current input networks. The current input network on the PM4104APDA has been set up for a shunt with input resistors RC = 200W. The filtering capacitors have been set to CC = 100nF for simplicity. The resulting cut-off frequency is 15.9kHz. Voltage Sense Input Network The voltage input network on the PM4104APDA has been designed for operation at both 220V and 110V mains voltage. The mains voltage is selected by means of a jumper (J1). The voltage input network attenuates the mains voltage signal to a lower voltage by means of a voltage divider. A trimpot is used to tap this voltage divider at different levels to effect calibration. Figure 4 shows the voltage sense input network as implemented on the PM4104APDA. The voltage sense input of the SA4104A/B saturates at an input current of ±17.6μARMS (±25μAPEAK). The current into the voltage sense input should therefore be set between 11μARMS and 12μARMS at nominal mains voltage (VNOM) to allow for a mains voltage variation of up to +30% and –50% without saturating the voltage sense input. The input resistor R12 sets the current input into the device. This resistor should not be too large else the capacitor for the low-pass filter will be quite small. This could cause inaccurate phase shift due to parasitic capacitances and affect the performance of the energy meter at low power factor. Therefore R12 = 100k W is chosen. For the purpose of the evaluation module a very large tuning range on the trimpot is selected, so let R11 and P1 be 1k W each and the voltage over the combination of R11 and P1 be 1.76V. This allows the input currents on the voltage sense inputs of the device to be scaled from 17.6μARMS down to 8.8μARMS. The following equations can be used to obtain the remaining resistor values: W + + + + W = k 2 10 R 9 R 8 R 7 R k 2 V 220 V 76 . 1 and W + + W = k 2 8 R 7 R k 2 V 110 V 76 . 1 This results in R7 + R8 = 123k W and R9 + R10 = 125kW and the values are chosen as R7 = 75k W, R8 = 47kW and R9 = R10 = 62k W. The effect of R12 can be ignored in the above equations, given the fact that R12 is significantly larger than the combination of P1 and R11. A low-pass filter is required on the voltage sense input to remove any high frequency signals that could affect the performance of the SA4104A/B. If a current transformer is used as a current sensing element then this low pass filter is used to compensate for the phase shift of the current transformer as well by purposefully increasing the cut-off frequency. R12 R9 IVP GND C3 R8 R7 GND V NOM (220V / 110V) (11µA RMS) Live Neutral GND R11 P1 SA4104A SA4104B AGND JS2 “L” JS2 “N” R10 GND J1 110V / 220V R12 R9 IVP GND C3 R8 R7 GND V NOM (220V / 110V) (11µA RMS) Live Neutral GND R11 P1 SA4104A SA4104B AGND JS2 “L” JS2 “N” R10 GND J1 110V / 220V Figure 4: Voltage input network on the PM4104APDA |
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