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Applying Fouriers law of heat conduction to the fuel

Fourier s law states that the heat flow, t (W), is proportional to the area of flow, A (m ), and the temperature gradient, dT/dx (K/m). In one dimension, this may be written  [Pg.369]

It may be shown (Rogers and Mayhew, 1992) that applying Fourier s law to heat conduction in a three-dimensional solid subject to a distributed internal heat source produces the following equation characterizing the steady state  [Pg.369]

Its cylindrical nature means that cylindrical coordinates are the most convenient for analysing heat conduction in the fuel pin. A formal statement of equation (A8.4) [Pg.369]

Integrating equation (A8.6) with respect to radial distance, r, gives  [Pg.370]

Physically, we know that the maximum temperature will occur at the centre of the pin, i.e. at r = 0, implying (dr,/dr)(0) = 0. Substituting these conditions into equation (A8.7) shows that the constant of integration must be zero. Hence [Pg.370]




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