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MR751RLG Datasheet(PDF) 5 Page - ON Semiconductor |
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MR751RLG Datasheet(HTML) 5 Page - ON Semiconductor |
5 / 7 page MR750 SERIES http://onsemi.com 5 Figure 9. Rectification Efficiency Figure 10. Reverse Recovery Time REPETITION FREQUENCY (kHz) 2.0 1.0 100 50 30 20 70 3.0 5.0 100 70 7.0 10 20 30 50 TJ = 25°C CURRENT INPUT WAVEFORM IR/IF, RATIO OF REVERSE TO FORWARD CURRENT 0.2 0.1 20 7.0 5.0 2.0 1.0 7.0 0.3 0.5 10 3.0 10 0.7 1.0 2.0 3.0 5.0 TJ = 25°C IF = 5 A 3 A 1 A IF 0 IR trr Figure 11. Junction Capacitance Figure 12. Forward Recovery Time VR, REVERSE VOLTAGE (VOLTS) 1.0 3.0 500 300 200 100 70 50 2.0 10 20 100 7.0 5.0 50 30 TJ = 25°C 1.0 IF, FORWARD PULSE CURRENT (AMP) 0.7 0.5 0.3 0.2 0.1 2.0 5.0 3.0 1.0 7.0 10 ufr = 1.0 V TJ = 25°C ufr uf tfr TJ = 175°C 30 700 1000 30 20 10 70 ufr = 2.0 V RS RL VO Figure 13. Single−Phase Half−Wave Rectifier Circuit The rectification efficiency factor σ shown in Figure 9 was calculated using the formula: σ + P(dc) P(rms) + V2o(dc) R L V2o(rms) RL .100% + V2o(dc) V2o(ac) ) V2o(dc) .100% (1) For a sine wave input Vm sin (wt) to the diode, assumed lossless, the maximum theoretical efficiency factor becomes: σ (sine) + V2m p2RL V2m 4RL .100% + 4 π2 .100% + 40.6% (2) For a square wave input of amplitude Vm, the efficiency factor becomes: σ (square) + V2m 2RL V2m RL .100% + 50% (3) (A full wave circuit has twice these efficiencies) As the frequency of the input signal is increased, the reverse recovery time of the diode (Figure 10) becomes significant, resulting in an increasing AC voltage component across RL which is opposite in polarity to the forward current, thereby reducing the value of the efficiency factor σ, as shown on Figure 9. It should be emphasized that Figure 9 shows waveform efficiency only; it does not provide a measure of diode losses. Data was obtained by measuring the AC component of Vo with a true rms AC voltmeter and the DC component with a DC voltmeter. The data was used in Equation 1 to obtain points for Figure 9. |
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