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author | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
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committer | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
commit | 7f60ea012dd2524dae921a2a35adbf7ef21f2bb6 (patch) | |
tree | dbb9e3ddb5fc829e7c5c7e6be99b2c4ba356132c /3547/CH5/EX5.1 | |
parent | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (diff) | |
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-rw-r--r-- | 3547/CH5/EX5.1/Ex5_1.sce | 34 |
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diff --git a/3547/CH5/EX5.1/5_1.jpg b/3547/CH5/EX5.1/5_1.jpg Binary files differnew file mode 100644 index 000000000..1d6bbdd2d --- /dev/null +++ b/3547/CH5/EX5.1/5_1.jpg diff --git a/3547/CH5/EX5.1/Ex5_1.sce b/3547/CH5/EX5.1/Ex5_1.sce new file mode 100644 index 000000000..3278fded7 --- /dev/null +++ b/3547/CH5/EX5.1/Ex5_1.sce @@ -0,0 +1,34 @@ +// Example no.5.1
+// To calculate (a) the photon incidence rate, (b) the photon absorption rate, and, (c) the quantum efficiency.
+// Page no.196
+
+clc;
+clear all;
+// Given data
+lambda=550*10^(-9); // The wavelength of electromagnetic wave in m
+c=3*10^8; // Speed of ligth in air
+h=6.626*10^(-34); // Planck's constant
+alpha=10^4; // absorption coefficient
+W=3*10^-4; // width of the active region
+Pi=1*10^-9; // optical power
+eta=0.9; // the fraction of photocarriers that contribute to the photocurrent
+Rp=0; // the power transmission coefficient at the air–semiconductor interface
+
+// (a) the photon incidence rate
+Eph=(h*c)/lambda; // The energy of a photon
+Rincident=Pi/Eph; // The photon incidence rate
+
+// Display result on command window
+printf('\n The photon incidence rate = %0.2f X 10^9 photon/s',Rincident*10^-9);
+
+// (b) the photon absorption rate
+Rabs=(Rincident*(1-exp(-alpha*W))); // The photon absorption rate
+
+// Display result on command window
+printf('\n The photon absorption rate = %0.2f X 10^9 photon/s',Rabs*10^-9)
+
+//c) the quantum efficiency
+neta=(1-Rp)*eta*(1-exp(-alpha*W)); // The quantum efficiency
+
+// Display result on command window
+printf('\n The quantum efficiency = %0.3f',neta)
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