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LTM4643 Datasheet(PDF) 14 Page - Analog Devices |
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LTM4643 Datasheet(HTML) 14 Page - Analog Devices |
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14 / 24 page ![]() LTM4705 14 Rev. 0 For more information www.analog.com APPLICATIONS INFORMATION mounted to a JESD 51-9 defined test board, which does not reflect an actual application or viable operat- ing condition. 2. θJCbottom, the thermal resistance from junction to the bottom of the product case, is determined with all of the component power dissipation flowing through the bottom of the package. In the typical μModule regulator, the bulk of the heat flows out the bottom of the package, but there is always heat flow out into the ambient environment. As a result, this thermal resistance value may be useful for comparing pack- ages but the test conditions don’t generally match the user’s application. 3. θJCtop, the thermal resistance from junction to top of the product case, is determined with nearly all of the component power dissipation flowing through the top of the package. As the electrical connections of the typical µModule are on the bottom of the package, it is rare for an application to operate such that most of the heat flows from the junction to the top of the part. As in the case of θJCbottom, this value may be useful for comparing packages but the test conditions don’t generally match the user’s application. 4. θJB, the thermal resistance from junction to the printed circuit board, is the junction-to-board thermal resistance where almost all of the heat flows through the bottom of the µModule and into the board, and is really the sum of the θJCbottom and the thermal resistance of the bottom of the part through the solder joints and through a portion of the board. The board temperature is measured a specified distance from the package, using a two sided, two layer board. This board is described in JESD 51-9. A graphical representation of the aforementioned ther- mal resistances is given in Figure 7; blue resistances are contained within the μModule regulator, whereas green resistances are external to the µModule. As a practical matter, it should be clear to the reader that no individual or sub-group of the four thermal resistance parameters defined by JESD 51-12 or provided in the Pin Configuration section replicates or conveys normal operating conditions of a μModule. For example, in nor- mal board mounted applications, never does 100% of the device’s total power loss (heat) thermally conduct exclusively through the top or exclusively through bottom of the µModule—as the standard defines for θJCtop and θJCbottom, respectively. In practice, power loss is ther- mally dissipated in both directions away from the pack- age—granted, in the absence of a heat sink and airflow, a majority of the heat flow is into the board. Within a SIP (system-in-package) module, be aware there are multiple power devices and components dissipating power, with a consequence that the thermal resistances relative to different junctions of components or die are not exactly linear with respect to total package power loss. To reconcile this complication without sacrificing modeling simplicity—but also, not ignoring practical realities—an approach has been taken using FEA software modeling along with laboratory testing in a controlled environment chamber to reasonably define and correlate the thermal resistance values supplied in this data sheet: (1) Initially, FEA software is used to accurately build the mechanical geometry of the µModule and the specified PCB with all of the correct material coefficients along with accurate power loss source definitions; (2) this model simulates a software-defined JEDEC environment consistent with JSED51-9 to predict power loss heat flow and tempera- ture readings at different interfaces that enable the cal- culation of the JEDEC-defined thermal resistance values; (3) the model and FEA software is used to evaluate the µModule with heat sink and airflow; (4) having solved for and analyzed these thermal resistance values and simu- lated various operating conditions in the software model, a thorough laboratory evaluation replicates the simulated conditions with thermocouples within a controlled-envi- ronment chamber while operating the device at the same power loss as that which was simulated. An outcome of this process and due-diligence yields a set of derating curves provided in other sections of this data sheet. After these laboratory test have been performed and correlated to the µModule model, then the θJB and θBA are summed together to correlate quite well with the µModule model with no airflow or heat sinking in a properly define cham- ber. This θJB + θBA value is shown in the Pin Configuration |
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