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-rw-r--r--3655/CH3/EX3.1/Ex3_1.pngbin0 -> 41200 bytes
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-rw-r--r--3655/CH3/EX3.4/Ex3_4.sce24
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diff --git a/3655/CH3/EX3.1/Ex3_1.png b/3655/CH3/EX3.1/Ex3_1.png
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diff --git a/3655/CH3/EX3.1/Ex3_1.sce b/3655/CH3/EX3.1/Ex3_1.sce
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+// Example 3.1
+// Computation for mobility of the free electrons in aluminium//
+// Page no.61
+
+clc;
+clear;
+close;
+
+//Given data ;
+d=2.70*10^3//2.70*10^3 kg/m3
+v=3;//3 electrons/atom
+A=26.98;
+M=1.660*10^-27;//1.660*10^-27 kg/atom
+e=1.60*10^-19;
+R=3.44*10^-8;//R=resistivity
+
+//...................................(B)....................................//
+
+//Calculation for concentration of the free electrons in aluminium//
+n=(d*v)/(A*M);
+
+//Calculation for mobility of the free electrons in aluminium//
+mu=10^4/(n*e*R);//mu=mobility of the free electrons
+
+
+
+//Displaying the result in command window
+printf('\n Concentration of the free electrons in aluminium = %0.3f x 10^29 electron/m3',n*10^-29);
+printf('\n \n Mobility of the free electrons in aluminium = %0.2f cm2/V sec',mu);
+
+
+
+//Answers are varying due to round off error//
diff --git a/3655/CH3/EX3.3/Ex3_3.png b/3655/CH3/EX3.3/Ex3_3.png
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diff --git a/3655/CH3/EX3.3/Ex3_3.sce b/3655/CH3/EX3.3/Ex3_3.sce
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+// Example 3.3
+// Computation for numerical value of n and EF//
+// Page no.71
+
+clc;
+clear;
+close;
+
+//Given data ;
+A_num=6.02*10^23;//Avogadro number
+atom_wt=184;//Atomic weight
+sg=18.8;//specific gravity of tungstan
+n_elect=2;//number of electrons
+n_atom=1;//number of atom per molecule
+
+
+//Calculation for numerical value of n//
+n=(A_num*(1/atom_wt)*sg*n_elect*n_atom)*10^6;
+
+//Calculation for numerical value of EF//
+EF=3.64*10^-19*n^(2/3);
+
+
+//Displaying the result in command window
+printf('\n Numerical value of n = %0.2f x 10^29 electron/m3',n*10^-29);
+printf('\n \n Numerical value of EF = %0.2f eV',EF);
+
+
+//Answers are varying due to round off error//
diff --git a/3655/CH3/EX3.4/Ex3_4.png b/3655/CH3/EX3.4/Ex3_4.png
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diff --git a/3655/CH3/EX3.4/Ex3_4.sce b/3655/CH3/EX3.4/Ex3_4.sce
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+// Example 3.4
+// Computation for percentage of electrons leaving a tungstan filament which can surmount a barrier of height 1eV//
+// Page no.78
+
+clc;
+clear;
+close;
+
+//Given data ;
+Vr=1;
+VT=2700/11600;//VT=T/11600
+
+
+//Calculation for percentage of electrons leaving a tungstan filament at 2700 degree K//
+P1=(exp(-Vr/VT))*100;//P1=I/Ith
+
+//Hence only about 1.4% of the electrons have surface-directed energies in excess of 1eV//
+
+
+//Displaying the result in command window
+printf('\n Percentage of electrons leaving a tungstan filament which can surmount a barrier of height 1eV = %0.1f percent',P1);
+
+
+//Answers are varying due to round off error//
diff --git a/3655/CH3/EX3.5/Ex3_5.png b/3655/CH3/EX3.5/Ex3_5.png
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diff --git a/3655/CH3/EX3.5/Ex3_5.sce b/3655/CH3/EX3.5/Ex3_5.sce
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+// Example 3.5
+// Computation for percentage increase in zero-external-field thermoinic-emission current because of the schottky effect//
+// Page no.78
+
+clc;
+clear;
+close;
+
+//Given data ;
+V=500;//plate voltage
+ra=1;//anode radius
+rk=0.01;//cathode radius
+r=10^-4;
+T=2500;
+
+
+
+//Calculation for electric field intensity at the surface of the cathode//
+E=(V/(log(ra/rk)))*(1/r);
+
+//Calculation for percentage increase in zero-external-field thermoinic-emission current because of the schottky effect//
+P1=log(%e^((0.434*0.44*E^(1/2))/T));//P1=log(I/Ith)
+P2=10^0.0796;//P2=I/Ith
+
+//I/Ith=1.20,shows that the schottky theory predicts a 20 percent increase over the zero-field emission current//
+
+
+//Displaying the result in command window
+printf('\n Electric field intensity at the surface of the cathode = %0.3f x 10^6 V/m',E*10^-6);
+printf('\n \n log(I/Ith) = %0.4f ',P1);
+printf('\n \n I/Ith = %0.2f ',P2);
+printf("\n \n \n \n I/Ith=1.20,shows that the Schottky theory predicts a 20 percent increase over the zero-field emission current.");
+
+//Answers are varying due to round off error//