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Diffstat (limited to '1309/CH11/EX11.3/ch11_3.sce')
-rwxr-xr-x | 1309/CH11/EX11.3/ch11_3.sce | 24 |
1 files changed, 24 insertions, 0 deletions
diff --git a/1309/CH11/EX11.3/ch11_3.sce b/1309/CH11/EX11.3/ch11_3.sce new file mode 100755 index 000000000..df7ae08a2 --- /dev/null +++ b/1309/CH11/EX11.3/ch11_3.sce @@ -0,0 +1,24 @@ +clc; +clear; +printf("\t\t\tChapter11_example3\n\n\n"); +// (a) Calculation of the emissivity of the hole.(b) the rate of radiant emission from the hole +D=2.5/12; // diameter in ft +L=4.5/12; // length in ft +A=(2*%pi*D^2/4)+(%pi*D*L); +printf("\nThe inside surface area is %.3f sq.ft ",A); +A_hole=%pi*(1/(8*12))^2/4; +printf("\nThe area of a 1/8 inch hole is %.3e sq.ft",A_hole); +f=A_hole/A; // fraction of area removed +printf("\nThe fraction of area removed is %.3e ",f); +printf("\n\n\t\t\tSolution to Part (a)\n"); +// for rolled and polished aluminum, that emissivity = 0.039 from appendix table E1 +emissivity=0.039; +emissivity_hole=emissivity/(emissivity+(1-emissivity)*f); +printf("\nThe emissivity of the hole is %.4f",emissivity_hole); +printf("\n\n\t\t\tSolution to Part (b)\n"); +sigma=0.1714e-8; // stefan Boltzmann constant in BTU/(hr~ft^2 degree R) +T=150+460; // temperature in degree R +qe=emissivity_hole*sigma*T^4; +printf("\nThe heat lost per unit area of the hole is %d BTU/hr",qe); +Qe=A_hole*qe; +printf("\nThe heat lost by the hole is %.2e BTU/hr",Qe); |