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Diffstat (limited to '181/CH2/EX2.1')
-rwxr-xr-x | 181/CH2/EX2.1/example2_1.sce | 37 | ||||
-rwxr-xr-x | 181/CH2/EX2.1/example2_1.txt | 11 |
2 files changed, 48 insertions, 0 deletions
diff --git a/181/CH2/EX2.1/example2_1.sce b/181/CH2/EX2.1/example2_1.sce new file mode 100755 index 000000000..aa8f81892 --- /dev/null +++ b/181/CH2/EX2.1/example2_1.sce @@ -0,0 +1,37 @@ +// Calculate height of potential-energy barrier
+// Basic Electronics
+// By Debashis De
+// First Edition, 2010
+// Dorling Kindersley Pvt. Ltd. India
+// Example 2-1 in page 77
+
+clear; clc; close;
+
+// Given data
+rho1=1.5; // Resistivity of p-side of Ge diode in ohm-cm
+rho2=1; // Resistivity of n-side of Ge diode in ohm-cm
+e=1.6*10^-19; // Charge on an electron in C
+mu_p=1800; // Mobility of holes
+mu_n=3800; // Mobility of electrons
+
+// Calculation
+N_A=1/(rho1*e*mu_p);
+N_D=1/(rho2*e*mu_n);
+printf("(a) rho = 2 ohm-cm\n");
+printf("N_A=%0.2e /cm^3\n",N_A);
+printf("N_D=%0.2e /cm^3\n",N_D);
+printf("The height of the potential energy barrier is:\n");
+V_0=0.026*log((N_A*N_D)/(2.5*10^13)^2);
+printf("V_0=%0.3f eV\n\n",V_0);
+printf("(b)For silicon:\n");
+N_A1=1/(rho1*e*500);
+N_D1=1/(2*e*1300);
+printf("N_A=%0.2e /cm^3\n",N_A1);
+printf("N_D=%0.2e /cm^3\n",N_D1);
+V_01=0.026*log((N_A1*N_D1)/(1.5*10^10)^2);
+printf("The height of the potential energy barrier is:\n");
+printf("V_0=%0.3f eV",V_01);
+
+// Result
+// (a) For Ge, V_0 = 0.226 eV
+// (b) For Si, V_0 = 0.655 eV
diff --git a/181/CH2/EX2.1/example2_1.txt b/181/CH2/EX2.1/example2_1.txt new file mode 100755 index 000000000..2f658283f --- /dev/null +++ b/181/CH2/EX2.1/example2_1.txt @@ -0,0 +1,11 @@ +(a) rho = 2 ohm-cm
+N_A=2.31e+015 /cm^3
+N_D=1.64e+015 /cm^3
+The height of the potential energy barrier is:
+V_0=0.227 eV
+
+(b)For silicon:
+N_A=8.33e+015 /cm^3
+N_D=2.40e+015 /cm^3
+The height of the potential energy barrier is:
+V_0=0.656 eV
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