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AN4022 数据表(PDF) 5 Page - STMicroelectronics |
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AN4022 数据表(HTML) 5 Page - STMicroelectronics |
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5 / 15 page ![]() DocID022589 Rev 2 5/15 AN4022 Dynamic resistance and how to measure it 15 2 Dynamic resistance and how to measure it In the previous section it was shown that the remaining voltage across a circuit to protect is closely linked to the VBR of the protection device used and to its dynamic resistance RD. The first parameter is generally well known and specified. In the past dynamic resistance has been specified but with test conditions different from real surge conditions giving pessimistic results, especially for short surges like electrostatic discharges. The pulse used had a duration of 2.5 µs. To be closer to typical ESD (defined in IEC61000-4-2), a 100 ns pulse width has been chosen. An accurate voltage measurement is quite difficult during high rate of rise current, due to the voltage probing loop inductance, inducing parasitic voltage: (). So a triangular pulse is used This is shown in Figure 6. No oscillations disturb the measurement. Figure 6. Current and voltage waveforms for RD measurement The current is measured during the test by a current monitor (Pearson Electronics). The voltage measurement is by the “Kelvin” method in coaxial configuration in order to get best accuracy (test board shown in Figure 7). An adequate voltage range and offset is set on the oscilloscope to get the best dynamic measurement without amplifier saturation. VPARASITIC =LPARASITIC × dl/dt IPP = 30 A tP 71 ns ≈ VCL value |
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