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AN441 数据表(PDF) 3 Page - STMicroelectronics |
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AN441 数据表(HTML) 3 Page - STMicroelectronics |
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3 / 16 page ![]() AN441 Reasons for inrush current in inductive loads Doc ID 3579 Rev 3 3/16 These two equations show that, when the inductive load is switched on in full-wave, the transient current depends on the Triac first turn-on delay with respect to the mains voltage zero point. Figure 2 shows the load current curve for triggering at zero voltage and triggering at the peak mains voltage. This figure comes from PSPICE simulation for a 150 ohm and 5 H load switched on at a voltage of 230 V rms at 50 Hz. Triggering at zero voltage brings the highest inrush current which can be up to twice the peak current reached in case of triggering at peak voltage. Figure 2. Inrush current difference according to Triac first turn-on delay Due to this high peak current, two problems may occur at AC switch level. ● High peak current may be higher than ITSM value (maximum surge peak current). In this case the component can be damaged. ● AC switch temperature may exceed the maximum allowed junction temperature (this will not lead necessarily to device failure but electrical parameters are not anymore guaranteed if working temperature is above max allowed value). Inrush currents have also to be checked to fit electromagnetic compatibility standards. Actually, IEC 61000-3-3 standard make it mandatory to limit inrush currents of appliances connected to the power network to reduce the flickering effect on lighting. It should also be noted that reducing inrush current helps to increase the reliability of the load and other switches or breakers used in series with the load. 1.2 Magnetic core saturation due to remanent induction In transient operation, the induction can follow a different path and reach the saturation value BS for which the magnetic field H increases very rapidly even for a low induction variation (see Figure 3). At saturation level the magnetic material permeability decreases drastically, down to air permeability. This leads to a lower inductance value. The load current is then mainly limited by the load resistance, and can increase substantially. Saturation then leads to a high increase of the coil current. -400 -300 -200 -100 0 100 200 300 400 0 20406080 100 Time (ms) -400 -300 -200 -100 0 100 200 300 400 Turn-on at zero crossing Turn-on at peak mains voltage Mains voltage |
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