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analysis of transient heat conduction in different geometries - ethesis ...

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Thus,<br />

a<br />

2<br />

Bθ<br />

=−<br />

2<br />

We can also write the second boundary condition as<br />

Us<strong>in</strong>g equation (3.55) , (3.58)and (3.60-3.61) we have<br />

Average temperature equation used <strong>in</strong> this problem is<br />

Substitut<strong>in</strong>g the value <strong>of</strong> θ we have<br />

Integrat<strong>in</strong>g equation (3.64) we have<br />

Substitut<strong>in</strong>g the value <strong>of</strong> 0 a , 1 a , 2 a we have<br />

29<br />

(3.60)<br />

∂ θ<br />

=− B( a0 + a1+ a2)<br />

∂ x<br />

(3.61)<br />

⎛ B ⎞<br />

a0 = θ ⎜1+ ⎟<br />

⎝ 2 ⎠ (3.62)<br />

1<br />

0 dx<br />

θ θ = ∫ (3.63)<br />

2<br />

( 0 1 2 )<br />

1<br />

∫ a a x a x dx<br />

0 (3.64)<br />

θ = + +<br />

a1 a2<br />

θ = a0<br />

+ +<br />

2 3<br />

Integrat<strong>in</strong>g non-dimensional govern<strong>in</strong>g equation we have<br />

(3.65)<br />

⎛ B ⎞<br />

θ = θ⎜1+ ⎟<br />

⎝ 3 ⎠ (3.66)<br />

∂θ ∂ θ<br />

dx dx Gdx<br />

∂τ∂x 2<br />

1 1 1<br />

= +<br />

0 0 2 0<br />

∫ ∫ ∫

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