| 전자부품 데이터시트 검색엔진 |
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L8150 데이터시트(PDF) 25 Page - STMicroelectronics |
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L8150 데이터시트(HTML) 25 Page - STMicroelectronics |
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25 / 37 page ![]() L8150 Precharge and hall effects filtering time description 25/37 Assumed this operation mode, it is easy to understand that as soon as the startup sequence is over, Hall effects commutations are filtered using a fraction of the electrical period given by the following equation, since T ∆ZC is equal to TEL when two consecutive zero-crossing signals generated by a rising edge on signal HallU are detected: ● Let's consider a startup sequence forced by FS comparator, supposing the motor rotating quickly in the direction imposed by the FR signal: Figure 15. Startup sequence forced by FS comparator, supposing the motor rotating quickly in the direction imposed by the FR signal: When the signal coming from the FS comparator has a falling edge, by default a zero- crossing signal is generated and the logic waits for a Hall effect commutation and applies to it a filtering time of TPRECHARGE=400µsec. The first significant zero-crossing signal is generated. Also the second Hall effect commutation is filtered using TPRECHARGE, after that the second zero-crossing signal is generated. Starting from the second Hall effect commutation, after the acquisition of the filtered Hall commutation, the logic outputs start applying the right pattern, and the motor is able to accelerate again. The next filtering time used for the Hall commutation is a fraction of the elapsed time between the first two Hall effect commutations, according to the previous TFILTER equation. This filtering time is used until the first rising edge on signal HallU is detected and a zero- crossing signal is generated. After that the filtering time used is a fraction of the elapsed time between the last two detected zero-crossing signals, in other words between the second Hall effect commutation and the rising edge on signal HallU. Finally, when the second rising edge on signal HallU is detected, the filtering time used is a fraction of the electrical period, as described in previous TFILTER-ROTATING equation. ● Let's consider a startup sequence forced by FS comparator, supposing the motor rotating quickly in the direction opposite to that imposed by the FR signal: T FILTER ROATING – 1 576 ---------- T ∆ ZC 1 576 ---------- T EL ⋅ = ⋅ = FS ZC HALL BUS FILTER TIME PHASES PHASES EXCITED T∆zc’’/576 T∆zc’ Tel U MOTOR ACCELERATING 400 us T∆zc’’ T∆zc’/576 T∆zc’/576 T∆zc’/576 T∆zc’’/576 400 us |
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