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Online proceedings - EDA Publishing Association

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11-13 <br />

May 2011, Aix-en-Provence, France<br />

<br />

Accurate Thermal Characterization of Power<br />

Semiconductor Packages by Thermal Simulation and<br />

Measurements<br />

Andras Vass-Varnai (1,2) , Robin Bornoff (2) , Sandor Ress (1,2) , Zoltan Sarkany (2) , Sandor Hodossy (1) , Marta Rencz (1,2)<br />

Budapest University of Technology and Economics (1)<br />

Mentor Graphics Mechanical Analysis Division (2)<br />

@eet.bme.hu<br />

@mentor.com<br />

In this paper the possibility of generating a compact thermal<br />

model based on thermal transient measurements is discussed and<br />

evaluated. A case study of a power diode in a cylindrical-shaped<br />

copper package is shown. The detailed model of the package is<br />

built and simulated in a CFD based thermal simulator software.<br />

The measurement results are compared to the results of the<br />

simulations and after some model refinement we found good<br />

agreement. The compact model of the package is also identified<br />

based on the structure functions generated from the real<br />

measurement. The case-node is determined using the standard<br />

dual-interface method. The resulting compact model has proven<br />

to be a perfect representation of the real package as the structure<br />

functions generated based on measurements and corresponding<br />

simulation results match perfectly.<br />

I. INTRODUCTION<br />

As the functionality of thermal simulators gets more and<br />

more complex, measurement techniques also improve.<br />

Thermal engineers face an increasingly difficult task to<br />

make the right selection from the existing tools. Beside this<br />

problem the precise determination of thermal performance<br />

indicators such as RthJC or RthJB is becoming more and<br />

more difficult as the package geometries become more<br />

complex. The thermal characterization of novel power<br />

packages hosting a number of dies is a major issue where<br />

the standard definitions cannot be applied anymore [1,2].<br />

The answer to these challenges may lie in a combined<br />

measurement and simulation approach. Measurements yield<br />

a structure description of materials having different<br />

conductivities; simulation gives the clue as to what certain<br />

sections in the measured structure correspond to. TIM<br />

materials are very difficult to model, as neither their<br />

conductivity nor their thickness can be determined with<br />

high accuracy even by the designer of a given package.<br />

Well planned thermal measurements are suitable tools to<br />

measure the in-situ resistance of these materials so that they<br />

can be later on used for accurate model creation. Another<br />

example may be the junction-to-case thermal resistance<br />

measurement of power packages where the single R thJC<br />

value obtained by measurements may not be a perfect<br />

indicator due to the complex heat-spreading path. In such<br />

cases steady-state simulations may show the temperature<br />

variation on the case surface which is a good basis to verify<br />

whether the simple R thJC approach is valid for the given<br />

package or not.<br />

As the measurement and simulation techniques mutually<br />

support each-other, the ultimate solution for package<br />

thermal characterization may be the simulation model<br />

creation based on real measurements [3].<br />

II. Experimental<br />

In order to compare simulation results with actual<br />

measurements a power diode package was selected having a<br />

cylindrical package shape and a hexagonal silicon diode<br />

inside.<br />

Fig. 1: Package structure of the studied diode (actual on left, 3D model on<br />

right)<br />

The package is app. 8.4 mm high and has a 12.5 mm<br />

diameter cooling surface on its bottom. The hexagonal die is<br />

located in the top region of the package and it is mounted<br />

using a top and bottom die attach layer to the copper<br />

cylinders. The edges of the hexagon are located on a 8.1<br />

324

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