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author | priyanka | 2015-06-24 15:03:17 +0530 |
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committer | priyanka | 2015-06-24 15:03:17 +0530 |
commit | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (patch) | |
tree | ab291cffc65280e58ac82470ba63fbcca7805165 /1309/CH6/EX6.1/ch6_1.sce | |
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diff --git a/1309/CH6/EX6.1/ch6_1.sce b/1309/CH6/EX6.1/ch6_1.sce new file mode 100755 index 000000000..96510720a --- /dev/null +++ b/1309/CH6/EX6.1/ch6_1.sce @@ -0,0 +1,36 @@ +clc; +clear; +printf("\t\t\tChapter6_example1\n\n\n"); +// Determination of the fluid outlet tetnperature and the tube-wall temperature at the outlet. +// properties of ethylene glycol at 20 degree celsius from appendix table C5 +Cp_20=2382; +rou_20=1.116*1000; +v_20=19.18e-6; +kf_20=.249; +a_20=.939e-7; +Pr_20=204; +// specifications of 1/2 standard type M seamless copper water tubing from appendix table F2 +OD=1.588/100; +ID=1.446/100; +A=1.642e-4; +Q=3.25e-6; +V=Q/A; +printf("\nThe average flow velocity is %.1f m/s",V*100); +// calculation of Reynold's Number to check flow regime +Re=V*ID/v_20; +printf("\nThe Reynolds Number is %.1f",Re); +// since Re>he 2100, the flow regime is laminar and the hydrodynamic length can be calculated as +Z_h=0.05*ID*Re; +printf("\nThe hydrodynamic length is %.1f cm",Z_h*100); +Tbi=20; // bulk-fluid inlet temperature in degree celsius +qw=2200; // incident heat flux in W/m^2 +L=3; // Length of copper tube in m +R=ID/2; // inner radius in m +Tbo=Tbi+(2*qw*a_20*L)/(V*kf_20*R); +printf("\nThe bulk-fluid outlet temperature is %.1f degree celsius",Tbo); +// This result is based on fluid properties evaluated at 20°C. taken as a first approximation +Z_t=0.05*ID*Re*Pr_20; +printf("\nThe thermal entry length is %.1f m",Z_t); +Two=Tbo+(11*qw*ID)/(48*kf_20); // The wall temperature at outlet in degree celsius +printf("\nThe wall temperature at outlet is %.1f degree celsius",Two); +//The result is based on first approximation based on flow properties evaluated at the fluid inlet temperature. |