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3.3.1.2 Heat balance at the outer surface of the heating plate<br />

Figure 3.9 Heating plate heat balance<br />

The heat generated by the heating element transfers to the heating plate (Figure 3.5).<br />

The thermal conduction resistance for each of these components can be expressed as:<br />

l<br />

R <br />

k A<br />

47<br />

(3.19)<br />

The overall resistance from heating element to heating plate is added up in table below:<br />

Table 3.2 Overall resistance from heating element to heating plate [19]<br />

Component<br />

l(m)<br />

(Thickness)<br />

k[W/(m·K)]<br />

(Thermal<br />

conductivity)<br />

A(m²)<br />

(Area)<br />

R(K/W)<br />

(Thermal<br />

resistance)<br />

Ceramic substrate 0.000635 24 0.0025 0.01058<br />

3M thermal conductive tape 0.00025 0.6 0.00567 0.07349<br />

Aluminium heating plate 0.0012 237 0.01033 0.00049<br />

Total from Ceramic to Plate 0.08456<br />

The heat balance on the top of the heating plate can be written as (Figure 3.9):<br />

(3.20)<br />

QHE QBw QHp T T<br />

HE Hp<br />

HE <br />

(3.21)<br />

RHS<br />

Q<br />

Because of the assumption that the ambient air is quiescent, the model is simplified to<br />

have only natural convection on all the outer surface area. For the outer circumferential<br />

vertical surface of the heating plate, the rim (Figure 3.9), Sparrow and Gregg have<br />

demonstrated that a vertical cylinder can be considered as flat vertical plate for the

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