Radiation across an annular gap

Input(s)

T1T_{1}: Temperature at Cylinder 1( K)1(\mathrm{~K})

T2T_{2}: Temperature at Cylinder 2( K)2(\mathrm{~K})

e1e_{1}: Emissivity at Cylinder 1 (fraction)

e2e_{2}: Emissivity at Cylinder 2 (fraction)

A1A_{1}: Area at Cylinder 1(ft)1(\mathrm{ft})

A2A_{2}: Area at Cylinder 2(ft)2(\mathrm{ft})

k\mathrm{k}: Stefan-Boltzmann Constant (BTU/hft2R4)\left(\mathrm{BTU} / \mathrm{h} \mathrm{ft}^{2}{ }^{\circ} \mathrm{R}^{4}\right)

Output(s)

Q: Heat Transfer Rate (BTU/h)(B T U / h)

Formula(s)

Q=k(( T14)(T24))(1 A1e1)+(1 A2)((1e2)1)\mathrm{Q}=\frac{\mathrm{k} *\left(\left(\mathrm{~T}_{1}^{4}\right)-\left(\mathrm{T}_{2}^{4}\right)\right)}{\left(\frac{1}{\mathrm{~A}_{1} * \mathrm{e}_{1}}\right)+\left(\frac{1}{\mathrm{~A}_{2}}\right) *\left(\left(\frac{1}{\mathrm{e}_{2}}\right)-1\right)}

Reference(s)

Bird, R.B., Stewart, W.E. and Lightfoot, E.N. (2002). Transport Phenomena (Second Ed.). John Wiley & Sons, Chapter: 16, Page: 494.

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