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AN4209 数据表(PDF) 9 Page - STMicroelectronics |
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AN4209 数据表(HTML) 9 Page - STMicroelectronics |
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9 / 19 page ![]() DocID023949 Rev 2 9/19 AN4209 STRVS parameters Figure 6. Thermal impedance variation of SMB package versus the pulse duration When the STRVS works under repetitive mode operation, the peak junction temperature Tjpeak must be below absolute rating Tjmax specified in the datasheet. For an infinite pulse train case, Tjpeak is expressed as shown in Equation 10: Equation 10 Note: The background average power PD has been subtracted, to avoid counting this effect twice in calculating temperature rise. In power conversion applications, two main cases occur. The time constants of the transient thermal impedance thermal must be considered regarding the switching period tSW in the application. Figure 7 illustrates the impact of operating frequency on the ripple temperature. The time constant of a thermal system is dependent on its transient thermal impedance curve. A sufficient estimation of thermal constant can be easily made from the simple RC thermal model representing the Zth(j-Ref) curve. Equation 11 Equation 12 Equation 12 applied to Figure 6 for an application working switching period tsw, around 10 µs, gives tau much greater than tsw due to the low value of Zth(@ 10 µs) before the Rth value. In this case the junction temperature rises and falls with a negligible dynamic temperature T j near Tjavg as shown in Figure 7. Since Tjpeak Tjavg, only the average junction temperature evaluation is needed using Equation 6. Notice that this case represents 90% of switch mode power supply applications (FSW > 20 kHz). Under these conditions, pulse widths are generally in the range of some tens to hundreds of nanoseconds and pulses may be viewed as a short block of constant power PSTEP, sustaining the junction temperature. 0.001 0.01 0.1 1 10 100 1000 0.000001 0.00001 0.0001 0.001 0.01 0.1 1 10 100 1000 10000 °C/W tp(s) ZTH(j-a) ZTH(j-l) Recommended pad layout Printed circuit board FR4, copper thickness = 35 µm l p l j TH D Step l j TH D p peak j T t Z P P R P t T+ · - + · = - - ) ( ) ( ) ( ) ( ) ( Zth(j-Ref)(t) = Rth(j-Ref) · (1 - e (-t/tau)) tau = -t(ln(1-Zth(t)/Rth) |
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