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A6263 датащи(PDF) 9 Page - Allegro MicroSystems |
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A6263 датащи(HTML) 9 Page - Allegro MicroSystems |
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9 / 11 page ![]() Protected LED Array Driver A6263 9 Allegro MicroSystems, LLC 115 Northeast Cutoff Worcester, Massachusetts 01615-0036 U.S.A. 1.508.853.5000; www.allegromicro.com Dissipation Limits There are two features limiting the power that can be dissipated by the A6263: thermal shutdown and thermal foldback. Thermal Shutdown If the thermal foldback feature is disabled by connecting the THTH pin to GND, or if the thermal resistance from the A6263 to the ambient environment is high, then the silicon temperature will rise to the thermal shutdown threshold and the current will be disabled. After the current is disabled the power dissipated will drop and the temperature will fall. When the temperature falls by the hysteresis of the thermal shutdown circuit, then the current will be re-enabled and the temperature will start to rise again. This cycle will repeat continuously until the ambient temperature drops or the A6263 is switched off. The period of this thermal shutdown cycle will depend on several electrical, mechanical, and thermal parameters, and could be from a few milliseconds to a few seconds. Thermal Foldback If there is a good thermal connection to the A6263, then the thermal foldback feature will have time to act. This will limit the silicon temperature by reducing the regulated current and therefore the dissipation. The thermal monitor will reduce the LED current as the temperature of the A6263 increases above the thermal monitor activation temperature, TJM. Thermal Dissipation The amount of heat that can pass from the silicon of the A6263 to the surrounding ambient environment depends on the thermal resistance of the structures connected to the A6263. The thermal resistance, RθJA, is a measure of the temperature rise created by power dissipation and is usually measured in degrees Celsius per watt (°C/W). The temperature rise, ΔT, is calculated from the power dissipated, PD, and the thermal resistance, RθJA, as: ΔT = PD × RθJA (9) A thermal resistance from silicon to ambient, RθJA, of approxi- mately 35°C/W can be achieved by mounting the A6263 on a standard FR4 double-sided printed circuit board (PCB) with a copper area of a few square inches on each side of the board under the A6263. Additional improvements in the range of 20% may be achieved by optimizing the PCB design. Optimizing Thermal Layout The features of the printed circuit board, including heat conduc- tion and adjacent thermal sources such as other components, have a very significant effect on the thermal performance of the device. To optimize thermal performance, the following should be taken into account: • The device exposed thermal pad should be connected to as much copper area as is available. • Copper thickness should be as high as possible (for example, 2 oz. or greater for higher power applications). • The greater the quantity of thermal vias, the better the dissipa- tion. If the expense of vias is a concern, studies have shown that concentrating the vias directly under the device in a tight pattern, as shown in figure 5, has the greatest effect. • Additional exposed copper area on the opposite side of the board should be connected by means of the thermal vias. The copper should cover as much area as possible. • Other thermal sources should be placed as remote from the device as possible Ø0.3 mm via Top-layer exposed copper Signal traces LJ package exposed thermal pad LJ package footprint 0.7 mm 0.7 mm Figure 5. Suggested PCB layout for thermal optimization (maximum available bottom-layer copper recommended) |
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