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AN2344 데이터시트(PDF) 12 Page - STMicroelectronics |
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AN2344 데이터시트(HTML) 12 Page - STMicroelectronics |
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12 / 27 page ![]() Datasheet avalanche ratings AN2344 12/27 have to be taken into consideration. These are mainly systemic in nature because the datasheet thermal impedance is the response of the userfs system to a rectangular power pulse, while maintaining the package case temperature at 25°C. This response can be expressed as follows: Equation 1 where, ∆TJC= Change in junction-case temperature ZthJC= Rectangular pulse derived from triangular pulse t= Triangular and Rectangular response time, and P= Power dissipated The application of Equation 1, without any modification cannot give precise information. In fact, a comparison between a rectangular and a triangular power pulse (both with the same peak), indicates that the peak temperature between them is quite different (see Figure 7.). To use the Zth, the triangular pulse can be approximated as rectangular pulse, with scaled amplitude and width. Another important concern about the use of thermal impedance is that usually it is experimentally and theoretically calculated according to the ON state of the device, so the normal power distribution within the device may be different from the one that occurs during the avalanche state. ST's approach to an EAS statement starts from a theoretical thermal model of the die with some experimental verifications. The TJ(max) during an avalanche may be sterting from: Equation 2 where: tAV = Avalanche time (s), A = die area (m2), P0 = peak power (W), and K= the silicon‘s thermal constant (Wm-2 s1/2 K-1) This solution is derived from the general heat transmission equation (Fourier equation) for the special case where an infinite media (mono-dimensional case) is subordinated to a short rectangular power source pulse and uniformly distributed over a die area. Equation 2, when it is applied to a triangular power pulse, is a simple and good approximation to use for the temperature increase calculation within the device during the avalanche operation, if the pulse is of short duration. ∆T jc Zth jc t ()P = T j P 0 AK -------- t av T starting + = |
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