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LP2995M 数据表(PDF) 8 Page - National Semiconductor (TI) |
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LP2995M 数据表(HTML) 8 Page - National Semiconductor (TI) |
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8 / 13 page ![]() Component Selection (Continued) the best solution when size and performance are critical, although their cost is typically higher than any other capaci- tor. Capacitor recommendations for different application circuits can be seen in the accompanying application notes with supporting evaluation boards. Thermal Dissipation Since the LP2995 is a linear regulator any current flow from V TT will result in internal power dissipation generating heat. To prevent damaging the part from exceeding the maximum allowable junction temperature, care should be taken to derate the part dependent on the maximum expected ambi- ent temperature and power dissipation. The maximum allow- able internal temperature rise (T Rmax) can be calculated given the maximum ambient temperature (T Amax)ofthe application and the maximum allowable junction temperature (T Jmax). T Rmax =TJmax −TAmax From this equation, the maximum power dissipation (P Dmax) of the part can be calculated: P Dmax =TRmax / θ JA The θ JA of the LP2995 will be dependent on several vari- ables: the package used; the thickness of copper; the num- ber of vias and the airflow. For instance, the θ JA of the SO-8 is 163˚C/W with the package mounted to a standard 8x4 2-layer board with 1oz. copper, no airflow, and 0.5W dissi- pation at room temperature. This value can be reduced to 151.2˚C/W by changing to a 3x4 board with 2 oz. copper that is the JEDEC standard. Figure 2 shows how the θ JA varies with airflow for the two boards mentioned. Layout is also extremely critical to maximize the output current with the LLP package. By simply placing vias under the DAP the θ JA can be lowered significantly. Figure 3 shows the LLP thermal data when placed on a 4-layer JEDEC board with copper thickness of 0.5/1/1/0.5 oz. The number of vias, with a pitch of 1.27 mm, has been increased to the maximum of 4 where a θ JA of 50.41˚C/W can be obtained. Via wall thickness for this calculation is 0.036 mm for 1oz. Copper. Additional improvements in lowering the θ JA can also be achieved with a constant airflow across the package. Main- taining the same conditions as above and utilizing the 2x2 via array, Figure 4 shows how the θ JA varies with airflow. 20039321 θ JA vs Airflow (SO-8) FIGURE 2. 20039322 LLP-16 θ JA vs # of Vias (4 Layer JEDEC Board)) FIGURE 3. 20039323 θ JA vs Airflow Speed (JEDEC Board with 4 Vias) FIGURE 4. www.national.com 8 |
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