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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 /581/CH11/EX11.11/Example11_11.sce | |
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diff --git a/581/CH11/EX11.11/Example11_11.sce b/581/CH11/EX11.11/Example11_11.sce new file mode 100755 index 000000000..ee67a382a --- /dev/null +++ b/581/CH11/EX11.11/Example11_11.sce @@ -0,0 +1,28 @@ +
+clear;
+clc;
+
+printf("\t Example 11.11\n");
+T1=300; //temp. of helium-water tube,K
+h=0.4; //height of vertical wall,m
+m=0.087*10^-3; //flow rate of helium,kg/(m^2*s)
+//this is a uniform flux natural convection problem.
+
+Mhes=0.01; // assuming the value of mass fraction of helium at the wall to be 0.01
+Mhef=Mhes/2; //film composition
+
+af=1.141; //film density,kg/m^3
+as=1.107; //wall density,kg/m^3
+Dha=7.119*10^-5; //diffusion coefficient,m^2/s
+u=1.857*10^5; //fil,m viscosity at 300K,kg/(m*s)
+Sc=(u/af)/Dha; //schimidt no.
+aa=1.177; //air density,kg/m^3
+Ra1=9.8*(aa-as)*m*h^4/(u*af*Dha^2*Mhes); //Rayleigh no.
+
+Nu=6/5*(Ra1*Sc/(4+9*Sc^0.5+10*Sc))^(1/5); //approximate nusselt no.
+s=m*h/(af*Dha*Nu); //average concentration of helium at hte wall
+
+//thus we have obtained an average wall concentration 14 oercent higher than our initial guess of Mhes.we repeat this calclations with revised values of densities to obtain Mhes = 0.01142
+
+printf(" average conentration of helium at the wall is 0.01142 ,since the result is within 0.5 percent of our second guess, a third iteration is not needed.");
+//end
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