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Development of a New Electro-thermal Simulation Tool for RF circuits

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20 2.2. Chip <strong>thermal</strong> model - mathematical considerations<br />

2.2.4. Thermal impedance<br />

Figure 2.7: Thermal impedance as a response to a step application <strong>of</strong> power, logarithmic<br />

time scale.<br />

From the definition, <strong>thermal</strong> impedance Zth is a response to a step application <strong>of</strong><br />

a power. Final value <strong>of</strong> <strong>thermal</strong> impedance always reaches steady state value Rth, as<br />

shown in Fig. 2.7.<br />

Since an equivalence <strong>of</strong> electrical and <strong>thermal</strong> quantities exists, a popular way to<br />

approximate the <strong>thermal</strong> impedance is by means <strong>of</strong> electrical <strong>thermal</strong> impedance, that<br />

is by an infinite amount <strong>of</strong> RC pairs. In this way, by means <strong>of</strong> electrical equivalence,<br />

Figure 2.8: Schematic pass from steady state to transient case.<br />

<strong>thermal</strong> phenomena can be described using circuit simulation environment. However,<br />

<strong>for</strong> computational reasons it is not possible to include infinite amount <strong>of</strong> RC pairs in a<br />

circuit simulator. The less amount <strong>of</strong> RC pairs is used, the better <strong>for</strong> a simulation time<br />

<strong>for</strong> a cost <strong>of</strong> accuracy. In these circumstances, a reasonable trade-<strong>of</strong>f must be found.<br />

A well known representation <strong>for</strong> <strong>thermal</strong> impedance is Foster (Fig. 2.9a) and Cauer<br />

(Fig. 2.9b) RC series. Both networks can be easily trans<strong>for</strong>med between each other<br />

[13].

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