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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 /405/CH8/EX8.1/8_1.sce | |
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-rwxr-xr-x | 405/CH8/EX8.1/8_1.sce | 33 |
1 files changed, 33 insertions, 0 deletions
diff --git a/405/CH8/EX8.1/8_1.sce b/405/CH8/EX8.1/8_1.sce new file mode 100755 index 000000000..ea50f6ba7 --- /dev/null +++ b/405/CH8/EX8.1/8_1.sce @@ -0,0 +1,33 @@ +clear;
+clc;
+printf("\t\t\tExample Number 8.1\n\n\n");
+// transmission and absorption in a gas plate
+// Example 8.1 (page no.-381)
+// solution
+
+T = 2000+273;// [K] furnace temperature
+L = 0.3;// [m] side length of glass plate
+t1 = 0.5;// transmissivity of glass between lambda1 to lambda2
+lambda1 = 0.2;// [micro m]
+lambda2 = 3.5;// [micro m]
+E1 = 0.3;// emissivity of glass upto lambda2
+E2 = 0.9;// emissivity of glass above lambda2
+t2 = 0;// transmissivity of glass except in the range of lambda1 to lambda2
+sigma = 5.669*10^(-8);// [W/square meter K^(4)]
+A = L^(2);// [square meter] area of glass plate
+// calculating constants to use table 8-1(page no.-379-380)
+K1 = lambda1*T;// [micro m K]
+K2 = lambda2*T;// [micro m K]
+// from table 8-1
+Eb_0_lam1_by_sigmaT4 = 0;
+Eb_0_lam2_by_sigmaT4 = 0.85443;
+Eb = sigma*T^(4);// [W/square meter]
+// total incident radiation is
+// for 0.2 micro m to 3.5 micro m
+TIR = Eb*(Eb_0_lam2_by_sigmaT4-Eb_0_lam1_by_sigmaT4)*A;// [W]
+TRT = t1*TIR;// [W]
+RA1 = E1*TIR;// [W] for 0<lambda<3.5 micro m
+RA2 = E2*(1-Eb_0_lam2_by_sigmaT4)*Eb*A;// [W] for 3.5 micro m <lambda< infinity
+TRA = RA1+RA2;// [W]
+printf("total energy absorbed in the glass is %f kW",TRA/1000);
+printf("\n\n total energy transmitted by the glass is %f kW",TRT/1000);
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