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

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Based on the <strong>analysis</strong> a closed form expression <strong>in</strong>volv<strong>in</strong>g temperature, <strong>heat</strong> source parameter,<br />

Biot number and time is obta<strong>in</strong>ed for a slab.<br />

3.3 TRANSIENT ANALYSIS ON A TUBE WITH SPECIFIED HEAT FLUX<br />

We consider the <strong>heat</strong> <strong>conduction</strong> <strong>in</strong> a tube <strong>of</strong> diameter 2R, <strong>in</strong>itially at a uniform temperature T0,<br />

hav<strong>in</strong>g <strong>heat</strong> flux at one side and exchang<strong>in</strong>g <strong>heat</strong> by convection at another side. A constant <strong>heat</strong><br />

transfer coefficient (h) is assumed on the other side and the ambient temperature (T∞) is assumed<br />

to be constant. Assum<strong>in</strong>g constant physical properties, k and α, the generalized <strong>transient</strong> <strong>heat</strong><br />

<strong>conduction</strong> valid for slab, cyl<strong>in</strong>der and sphere can be expressed as:<br />

∂T 1 ∂ ⎛ m ∂T<br />

⎞<br />

= α r m ⎜ ⎟<br />

∂t r ∂r⎝ ∂r<br />

⎠<br />

Where, m = 0 for slab, 1 and 2 for cyl<strong>in</strong>der and sphere, respectively. Here we have considered<br />

tube geometry. Putt<strong>in</strong>g m=1, equation (3.1) reduces to<br />

∂T 1 ∂ ⎛ ∂T<br />

⎞<br />

= α ⎜r⎟ ∂t r ∂r⎝ ∂r<br />

⎠ (3.23)<br />

Fig 3.2: Schematic <strong>of</strong> a tube with <strong>heat</strong> flux<br />

Subjected to boundary conditions<br />

∂ T<br />

k = −q"<br />

∂ r at<br />

r = R1<br />

23<br />

(3.24)

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