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