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author | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
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committer | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
commit | 7f60ea012dd2524dae921a2a35adbf7ef21f2bb6 (patch) | |
tree | dbb9e3ddb5fc829e7c5c7e6be99b2c4ba356132c /534/CH1/EX1.2/1_2_Emissive_Power_Irradiation.sce | |
parent | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (diff) | |
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Diffstat (limited to '534/CH1/EX1.2/1_2_Emissive_Power_Irradiation.sce')
-rw-r--r-- | 534/CH1/EX1.2/1_2_Emissive_Power_Irradiation.sce | 26 |
1 files changed, 26 insertions, 0 deletions
diff --git a/534/CH1/EX1.2/1_2_Emissive_Power_Irradiation.sce b/534/CH1/EX1.2/1_2_Emissive_Power_Irradiation.sce new file mode 100644 index 000000000..20610d7e4 --- /dev/null +++ b/534/CH1/EX1.2/1_2_Emissive_Power_Irradiation.sce @@ -0,0 +1,26 @@ +clear;
+clc;
+printf('FUNDAMENTALS OF HEAT AND MASS TRANSFER \n Incropera / Dewitt / Bergman / Lavine \n EXAMPLE 1.2 Page 11 \n')// Example 1.2
+// Find a) Emissive Power & Irradiation b)Total Heat Loss per unit length
+
+d=.07; //[m] - Outside Diameter of Pipe
+Ts = 200+273.15; //[K] - Surface Temperature of Steam
+Tsurr = 25+273.15; //[K] - Temperature outside the pipe
+e=.8; // Emissivity of Surface
+h=15; //[W/m^2.k] - Thermal Convectivity from surface to air
+stfncnstt=5.67*10^(-8); // [W/m^2.K^4] - Stefan Boltzmann Constant
+//Using Eq 1.5
+E = e*stfncnstt*Ts^4; //[W/m^2] - Emissive Power
+G = stfncnstt*Tsurr^4; //[W/m^2] - Irradiation falling on surface
+
+printf("\n (a) Surface Emissive Power = %.2f W/m^2",E);
+printf("\n Irradiation Falling on Surface = %.2f W/m^2",G);
+
+//Using Eq 1.10 Total Rate of Heat Transfer Q = Q by convection + Q by radiation
+q = h*(%pi*d)*(Ts-Tsurr)+e*(%pi*d)*stfncnstt*(Ts^4-Tsurr^4); //[W]
+
+printf("\n\n (b) Total Heat Loss per unit Length of Pipe= %.2f W",q);
+//END
+
+
+
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