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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 /3269/CH10/EX10.3/Ex10_3.sce | |
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diff --git a/3269/CH10/EX10.3/Ex10_3.sce b/3269/CH10/EX10.3/Ex10_3.sce new file mode 100755 index 000000000..c28ec2862 --- /dev/null +++ b/3269/CH10/EX10.3/Ex10_3.sce @@ -0,0 +1,41 @@ +// Example 10.3
+clear all;
+clc;
+
+// Given data
+E = 2; // Energy of gamma rays in MeV
+X_dot = 2.5; // Exposure rate in mR/hour
+phi0 = 10^9; // Intensity of gamma rays in gamma-rays/cm^2-sec from isotropic point source
+// Using the data from Table II.5 for 1 MeV
+mua_rho_air = 0.0238; // The ratio of total attenuation coefficient to density of air in cm^2/g
+phi_b = X_dot/(0.0659*E*mua_rho_air); // Buildup flux in gamma-rays/cm^2-sec
+
+// From standard data tables for concrete
+rho = 2.35; // Density of concrete in g/cm^3
+// Using the data from Table 10.3 for concrete at 2 MeV
+A1 = 18.089;
+A2 = 1-A1;
+alpha1 = -0.0425;
+alpha2 = 0.00849;
+// Using Eq 10.26
+printf(" \n The equation to calculate thickness is \n %.2E = (%E/2) *(%4.3f*E1(%4.3f*mu*a) %4.3f*E1(%4.3f*mu*a)) \n",phi_b,phi0,A1,(1+alpha1),A2,(1+alpha2));
+// Using the data from Table II.4 for E = 1 MeV for concrete
+mu_rho = 0.0445; // The ratio of total attenuation coefficient to density in cm^2/g
+mu = mu_rho*rho;
+// On solving the right hand side of equation
+// RHS = 1.13*10^7*(E1(0.9575*mu*a)-0.94*E1(1.00849*mu*a))
+// Let mu*a = x
+x = 1:20
+for i = 1:20
+ RHS(i) = 1.13*10^7*(exp(-0.9575*x(i))*((1/(0.9575*x(i))+(1/(0.9575*x(i))^3))) - exp(-1.00849*x(i))*((1/(1.00849*x(i))+(1/(1.00849*x(i))^3))));
+end
+plot2d("nl",x(:),RHS(:));
+xlabel("mu*a");
+ylabel("RHS");
+title("Semilog plot of RHS vs mu*a")
+// From the graph
+mua = 13.6; // This is the value when RHS = 1
+// Calculation
+a = mua/mu;
+// Result
+printf("\n The concrete thickness = %d cm \n",a);
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