1968
DOI: 10.1016/0029-5493(68)90028-9
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Unsteady heat conduction in finite hollow circular cylinders under time-dependent boundary conditions of the second kind

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1969
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Cited by 5 publications
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“…Following Ölçer and Sunderland, 58 the solution of eq 5 with initial condition eq 6 and boundary conditions eq 7 is where τ = 4 R 2 / D is a characteristic time constant (τ ∼ 5.57 ns with R = 1.5 nm and D = 1.21 × 10 –9 m 2 /s) and and δ 0 m is the Kronecker delta, J n ( x ) and Y n ( x ) are the n th order Bessel functions of the first kind and second kind, respectively, and β mn is the n th non-negative root of the following equation …”
Section: Resultsmentioning
confidence: 99%
“…Following Ölçer and Sunderland, 58 the solution of eq 5 with initial condition eq 6 and boundary conditions eq 7 is where τ = 4 R 2 / D is a characteristic time constant (τ ∼ 5.57 ns with R = 1.5 nm and D = 1.21 × 10 –9 m 2 /s) and and δ 0 m is the Kronecker delta, J n ( x ) and Y n ( x ) are the n th order Bessel functions of the first kind and second kind, respectively, and β mn is the n th non-negative root of the following equation …”
Section: Resultsmentioning
confidence: 99%