| 数据搜索系统,热门电子元器件搜索 |
|
ADP151ACBZ-1.8-R7 数据表(PDF) 15 Page - Analog Devices |
|
|
|||||||||||||||||||||||||||||
ADP151ACBZ-1.8-R7 数据表(HTML) 15 Page - Analog Devices |
|
15 / 24 page ![]() ADP151 Rev. 0 | Page 15 of 24 CURRENT LIMIT AND THERMAL OVERLOAD PROTECTION The ADP151 is protected against damage due to excessive power dissipation by current and thermal overload protection circuits. The ADP151 is designed to current limit when the output load reaches 300 mA (typical). When the output load exceeds 300 mA, the output voltage is reduced to maintain a constant current limit. Thermal overload protection is included, which limits the junction temperature to a maximum of 150°C (typical). Under extreme conditions (that is, high ambient temperature and power dissipation) when the junction temperature starts to rise above 150°C, the output is turned off, reducing the output current to 0. When the junction temperature drops below 135°C, the output is turned on again, and output current is restored to its nominal value. Consider the case where a hard short from VOUT to ground occurs. At first, the ADP151 current limits, so that only 300 mA is conducted into the short. If self-heating of the junction is great enough to cause its temperature to rise above 150°C, thermal shutdown activates, turning off the output and reducing the output current to 0. As the junction temperature cools and drops below 135°C, the output turns on and conducts 300 mA into the short, again causing the junction temperature to rise above 150°C. This thermal oscillation between 135°C and 150°C causes a current oscillation between 300 mA and 0 mA that continues as long as the short remains at the output. Current and thermal limit protections are intended to protect the device against accidental overload conditions. For reliable operation, device power dissipation must be externally limited so that junction temperatures do not exceed 125°C. THERMAL CONSIDERATIONS In most applications, the ADP151 does not dissipate much heat due to its high efficiency. However, in applications with high ambient temperature, high supply voltage to output voltage differential, the heat dissipated in the package is large enough that it can cause the junction temperature of the die to exceed the maximum junction temperature of 125°C. When the junction temperature exceeds 150°C, the converter enters thermal shutdown. It recovers only after the junction temperature has decreased below 135°C to prevent any permanent damage. Therefore, thermal analysis for the chosen application is very important to guarantee reliable performance over all conditions. The junction temperature of the die is the sum of the ambient temperature of the environment and the tempera- ture rise of the package due to the power dissipation, as shown in Equation 2. To guarantee reliable operation, the junction temperature of the ADP151 must not exceed 125°C. To ensure that the junction temperature stays below this maximum value, the user must be aware of the parameters that contribute to junction temperature changes. These parameters include ambient temperature, power dissipation in the power device, and thermal resistances between the junction and ambient air (θJA). The θJA number is dependent on the package assembly compounds that are used and the amount of copper used to solder the package GND pins to the PCB. Table 5 shows typical θJA values of the 5-lead TSOT package for various PCB copper sizes. Table 6 shows the typical ΨJB values of the 5-lead TSOT and 4-ball WLCSP. Table 5. Typical θJA Values Copper Size (mm2) θJA (°C/W) TSOT WLCSP 01 170 260 50 152 159 100 146 157 300 134 153 500 131 151 1 Device soldered to minimum size pin traces. Table 6. Typical ΨJB Values Model ΨJB (°C/W) TSOT 43 WLCSP 58 The junction temperature of the ADP151 can be calculated from the following equation: TJ = TA + (PD × θJA) (2) where: TA is the ambient temperature. PD is the power dissipation in the die, given by PD = [(VIN − VOUT) × ILOAD] + (VIN × IGND) (3) where: ILOAD is the load current. IGND is the ground current. VIN and VOUT are input and output voltages, respectively. Power dissipation due to ground current is quite small and can be ignored. Therefore, the junction temperature equation simplifies to the following: TJ = TA + {[(VIN − VOUT) × ILOAD] × θJA} (4) As shown in Equation 4, for a given ambient temperature, input- to-output voltage differential, and continuous load current, there exists a minimum copper size requirement for the PCB to ensure that the junction temperature does not rise above 125°C. Figure 37 to Figure 50 show junction temperature calculations for different ambient temperatures, load currents, VIN-to-VOUT differentials, and areas of PCB copper. |
|
|
链接网址 |
| ALLDATASHEET是否为您带来帮助? [ DONATE ] |
关于 Alldatasheet | 广告服务 | 联系我们 | 隐私政策 | 数据表链接 | 链接交换 | 制造商名单 All Rights Reserved©Alldatasheet.com |
| Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
|
Family Site : ic2ic.com |
icmetro.com |