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AN1172 Datasheet(PDF) 21 Page - STMicroelectronics |
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AN1172 Datasheet(HTML) 21 Page - STMicroelectronics |
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21 / 23 page ![]() AN1172 How to calculate the junction temperature during clamping periods 21/23 Figure 23. shows the maximum ∆Tj reached for different load RMS currents and power factors. Calculations are similar whatever the package is (TO92, DIL20, SOT223), because in such a range of times, the Zth is only due to the die area. Note that ∆Tj first increases. On this curve part, the load peak current is lower than the iH level (taken equal to its worst value: 60 mA). So, when the load RMS current increases, the turned-off current increases too. When the load peak current becomes higher than iH, ∆Tj decreases because of the load series inductance decrease (here the turn-off current is constant and equals iH). Figure 23. Supplementary temperature rise at clamping depending on load nature (for ACS402-5SB4 or ACS108-5SX) It can be concluded that, if the junction temperature was 110° C before turn-off, the maximum transient temperature can reach 160° C. As these events last less than one ms (refer to Figure 22.), such junction temperatures can be permitted. C.3 Repetitive clampings To evaluate heating due to repetitive clampings, Equation C6 can be used, assuming that the clampings occur at a constant period T and that the conduction losses can be neglected in front of the previous ones. Equation C6 In practice T (above 1s) is very much higher than the clamping duration. Equation C6 can then be simplified to the following one. Equation C7 60 45 cos =0.1 ϕ cos =0.7 ϕ cos =0.9 ϕ cos =0.98 ϕ 30 0 0.1 0.2 0.3 0.4 0.5 15 IRMS (A) ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ - + - - + ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ - - + - ⋅ = ∆ ) t t ( Zth ) T ( Zth ) t t T ( Zth T t t 1 Rth T t t I V 2 1 T 0 ZC 0 ZC 0 ZC 0 ZC H cl rep Rth T t t I V 2 1 T 0 ZC H cl rep - ⋅ = ∆ |
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