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VB409SP 数据表(PDF) 6 Page - STMicroelectronics |
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VB409SP 数据表(HTML) 6 Page - STMicroelectronics |
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6 / 9 page ![]() 6/9 VB409 / VB409SP 1 AVERAGE POWER CALCULATION IN WORST CASE As before explained, the device also senses the preregulator voltage (Vcap), so that as soon as the capacitor reaches its maximum voltage, the trilinton reduces the current so limiting furtherly power dissipation. On the contrary if the capacitor doesn’t reach the maximum value, the trilinton supplies current at a steady value (Imax) during the whole conduction angle. This is obviously the worst case, in which the average power dissipation is maximum. VIN t IIN ICL(in) Assuming that are the conduction angles, it results: As for t1: it follows: Where 0 t1 [, ] t2 T 2 --- [, ] = P AV 1 T -- VIN IIN ⋅ () t d 0 T ∫⋅ = = 1 T -- VIN ICL in () ⋅ () t d 0 t1 ∫ V IN I CL in () ⋅ () t d t2 T 2 -- ∫ + ⋅ ICL in () Vmax ⋅ T --------------------------- 2 π T ----- t ⋅ () sin t d 0 t1 ∫ 2 π T ----- t ⋅ () sin t d t2 T 2 --- ∫ + ⋅ == I CL in () V max ⋅ T --------------------------- 2 2 π T ----- t ⋅ () sin t d 0 t1 ∫ ⋅ = 2 I CL i n () Vmax ⋅ T --------------------------- T 2 π ----- 2 π T ----- t1 ⋅ () cos – 0 cos + [] ⋅⋅ = = = ICL in () V max ⋅ π --------------------------- 11 2 π T ----- t1 ⋅ () sin 2 – – ICL in () Vmax ⋅ π --------------------------- 11 V1 Vmax ---------- 2 – – ⋅ V 1 Vmax ---------- 2 π T ----- t1 ⋅ () sin = PAV = V1 vmax 0 t1 t2 T/2 T t V IN Vmax 2 π T ----- t ⋅ () sin ⋅ = 0 t T 2 --- ≤≤ T 2 --- tT ≤≤ 0 IIN ICL in () ⋅ = 0 tt1 ≤≤ t2 t T 2 -- ≤≤ 0 elsewhere V 1 Vref 1 1 R1 R2 -------- + () ⋅ = = Figure 3a Figure 3b t Vcap |
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