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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 /587/CH1/EX1.8 | |
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Diffstat (limited to '587/CH1/EX1.8')
-rwxr-xr-x | 587/CH1/EX1.8/example1_8.sce | 20 |
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diff --git a/587/CH1/EX1.8/example1_8.sce b/587/CH1/EX1.8/example1_8.sce new file mode 100755 index 000000000..56161439a --- /dev/null +++ b/587/CH1/EX1.8/example1_8.sce @@ -0,0 +1,20 @@ +clear;
+clc;
+
+//Example1.8[Measuring Convection Heat Transfer coefficient]
+//Given:-
+T_ambient=15;//Temperature of room[degree Celcius]
+T_surface=152;//Temperature of surface of wire[degree Celcius]
+L=2;//Length of wire[m]
+D=0.003;//Diameter of wire[m]
+V=60;//Voltage drop across the current wire[Volts]
+I=1.5;//Current flowing in the wire[amp]
+//Solution:-
+//When steady conditions are reached, the rate of heat loss from the wire equals the rate of heat generation in the wire as a result of resistance heating
+Q_=V*I;//[W]
+disp("W",Q_,"The rate of heat generated in the wire as a result of resistance heating is")
+As=%pi*D*L;//Surface Area of the wire[m^2]
+//Using Newton's Law of Cooling
+//and assuming all heat loss in wire to occur by convection
+h=Q_/(As*(T_surface-T_ambient));//[W/m^2.degree Celcius]
+disp("W/m^2.degree Celcius",h,"The convection Heat Transfer coefficient is" )
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