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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/CH2/EX2.11 | |
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Diffstat (limited to '587/CH2/EX2.11')
-rwxr-xr-x | 587/CH2/EX2.11/example2_11.sce | 22 |
1 files changed, 22 insertions, 0 deletions
diff --git a/587/CH2/EX2.11/example2_11.sce b/587/CH2/EX2.11/example2_11.sce new file mode 100755 index 000000000..ce3b24229 --- /dev/null +++ b/587/CH2/EX2.11/example2_11.sce @@ -0,0 +1,22 @@ +clear;
+clc;
+
+//Example2.11[Heat Conduction in a Plane Wall]
+//Given:-
+k_wall=1.2;//Thermal conductivity of wall[W/m.degree Celcius]
+L=0.2;//Thickness of wall[m]
+As=15;//Surface area[m^2]
+T1=120,T2=50;//The two sides of the wall are maintained at these constant temperatures[degree Celcius]
+//Solution (a)
+disp("Differential equation can be expressed as d^2(T)/(dx^2)=0")
+disp("with boundary conditions ")
+disp("degree Celcius",T1,"T(0)=T1=")
+disp("degree Celcius",T2,"T(L)=T2=")
+disp("integrating this we get,")
+disp("dT/dx=C1", ,"where C1 is an arbitrary constant")
+disp("integrating we obtain temperature to follow following relation :-")
+disp("and substituting values in above equation","T(x)=((T2-T1)/L)*x+T1 ")
+T3=(((T2-T1)/L)*(0.1))+T1;
+disp("degree Celcius",T3,"The value of temperature at x=0.1m is")
+Q_wall=-k_wall*As*((T2-T1)/L);//[W]
+disp("W",Q_wall,"The rate of heat conduction through the wall is")
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