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HCPL-M456 数据表(PDF) 13 Page - Agilent(Hewlett-Packard) |
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HCPL-M456 数据表(HTML) 13 Page - Agilent(Hewlett-Packard) |
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13 / 14 page ![]() 1-61 Figure 30. Waveforms for Dead Time Calculation. Figure 29. Minimum LED Skew for Zero Dead Time. VOUT1 VOUT2 ILED2 tPLH MAX. PDD* MAX. = (tPLH-tPHL) MAX. = tPLH MAX. - tPHL MIN. tPHL MIN. ILED1 Q1 ON Q2 OFF Q1 OFF Q2 ON *PDD = PROPAGATION DELAY DIFFERENCE NOTE: THE PROPAGATION DELAYS USED TO CALCULATE PDD ARE TAKEN AT EQUAL TEMPERATURES. VOUT1 VOUT2 ILED2 tPLH MIN. MAXIMUM DEAD TIME (DUE TO OPTOCOUPLER) = (tPLH MAX. - tPLH MIN.) + (tPHL MAX. - tPHL MIN.) = (tPLH MAX. - tPHL MIN.) - (tPLH MIN. - tPHL MAX.) = PDD* MAX. - PDD* MIN. tPHL MIN. ILED1 Q1 ON Q2 OFF Q1 OFF Q2 ON *PDD = PROPAGATION DELAY DIFFERENCE tPLH MAX. tPHL MAX. PDD* MAX. MAX. DEAD TIME NOTE: THE PROPAGATION DELAYS USED TO CALCULATE THE MAXIMUM DEAD TIME ARE TAKEN AT EQUAL TEMPERATURES. LED Drive Circuit Considerations for Ultra High CMR Performance Without a detector shield, the dominant cause of optocoupler CMR failure is capacitive coupling from the input side of the opto- coupler, through the package, to the detector IC as shown in Figure 20. The HCPL-4506, HCPL-0466 and HCNW4506 improve CMR performance by using a detector IC with an optic- ally transparent Faraday shield, which diverts the capacitively coupled current away from the sensitive IC circuitry. However, this shield does not eliminate the capacitive coupling between the LED and the optocoupler output pins and output ground as shown in Figure 21. This capacitive coupling causes perturbations in the LED current during common mode transients and becomes the major source of CMR failures for a shielded optocoupler. The main design objective of a high CMR LED drive circuit becomes keep- ing the LED in the proper state (on or off) during common mode transients. For example, the recommended application circuit (Figure 19), can achieve 15 kV/ µs CMR while minimizing component complexity. Note that a CMOS gate is recommended in Figure 19 to keep the LED off when the gate is in the high state. Another cause of CMR failure for a shielded optocoupler is direct coupling to the optocoupler output pins through CLEDO1 and CLEDO2 in Figure 21. Many factors influence the effect and magni- tude of the direct coupling includ- ing: the use of an internal or external output pull-up resistor, the position of the LED current setting resistor, the connection of the unused input package pins, and the value of the capacitor at the optocoupler output (CL). Techniques to keep the LED in the proper state and minimize the effect of the direct coupling are discussed in the next two sections. CMR with the LED On (CMRL) A high CMR LED drive circuit must keep the LED on during common mode transients. This is achieved by overdriving the LED current beyond the input threshold so that it is not pulled below the threshold during a transient. The recommended minimum LED current of 10 mA provides adequate margin over the maximum ITH of 5.0 mA (see Figure 5) to achieve 15 kV/ µs CMR. Capacitive coupling is higher when the internal load resistor is used (due to CLEDO2) and an IF = 16 mA is required to obtain 10 kV/ µs CMR. The placement of the LED current setting resistor effects the ability of the drive circuit to keep the LED on during transients and interacts with the direct coupling to the optocoupler output. For example, the LED resistor in Figure 22 is connected to the anode. Figure 23 shows the AC equivalent circuit for Figure 22 during common mode transients. During a +dVcm/dt in Figure 23, the current available at the LED anode (Itotal) is limited by the series resistor. The LED current (IF) is reduced from its DC value by an amount equal to the current that flows through CLEDP and CLEDO1. The situation is made worse |
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