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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 /1931/CH10 | |
download | Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.gz Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.bz2 Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.zip |
initial commit / add all books
Diffstat (limited to '1931/CH10')
-rwxr-xr-x | 1931/CH10/EX10.1/1.sce | 13 | ||||
-rwxr-xr-x | 1931/CH10/EX10.10/10.sce | 15 | ||||
-rwxr-xr-x | 1931/CH10/EX10.11/11.sce | 15 | ||||
-rwxr-xr-x | 1931/CH10/EX10.12/12.sce | 15 | ||||
-rwxr-xr-x | 1931/CH10/EX10.13/13.sce | 12 | ||||
-rwxr-xr-x | 1931/CH10/EX10.14/14.sce | 14 | ||||
-rwxr-xr-x | 1931/CH10/EX10.2/2.sce | 13 | ||||
-rwxr-xr-x | 1931/CH10/EX10.3/3.sce | 13 | ||||
-rwxr-xr-x | 1931/CH10/EX10.4/4.sce | 18 | ||||
-rwxr-xr-x | 1931/CH10/EX10.5/5.sce | 20 | ||||
-rwxr-xr-x | 1931/CH10/EX10.6/6.sce | 16 | ||||
-rwxr-xr-x | 1931/CH10/EX10.7/7.sce | 15 | ||||
-rwxr-xr-x | 1931/CH10/EX10.8/8.sce | 19 | ||||
-rwxr-xr-x | 1931/CH10/EX10.9/9.sce | 14 |
14 files changed, 212 insertions, 0 deletions
diff --git a/1931/CH10/EX10.1/1.sce b/1931/CH10/EX10.1/1.sce new file mode 100755 index 000000000..1ecac4b1d --- /dev/null +++ b/1931/CH10/EX10.1/1.sce @@ -0,0 +1,13 @@ +clc
+clear
+//INPUT DATA
+ec=4*10^-4//electrical conductivity of intrinsic silicon at room temperature in ohm^-1 m^-1
+me=0.14//The electron mobility in m^2 V^-1 s^-1
+mh=0.04//The hole mobility in m^2 V^-1 s^-1
+e=1.6*10^-19//charge of electron in coulombs
+
+//CALCULATION
+ni=(ec/(e*(me+mh)))/10^16//The intrinsic carrier concentration at room temperature in m^-3 *10^16
+
+//OUTPUT
+printf('The intrinsic carrier concentration at room temperature is %3.3f *10^16.m^-3 \n Since ne=nh=ni from law of mass action the electron and hole concentrations are 1.33*10^16.m^-3',ni)
diff --git a/1931/CH10/EX10.10/10.sce b/1931/CH10/EX10.10/10.sce new file mode 100755 index 000000000..af53d1aaf --- /dev/null +++ b/1931/CH10/EX10.10/10.sce @@ -0,0 +1,15 @@ +clc
+clear
+//INPUT DATA
+Eg=0.72*1.6*10^-19//The band gap of Ge in J
+T1=293//Temperature in K
+T2=313//Temperature in K
+x1=2//The conductivity of Ge at T1 in ohm^-1 m^-1
+e=1.6*10^-19//charge of electron in coulombs
+kb=1.38*10^-23//Boltzmann's constant m^2 Kg s^-2 k^-1
+
+//CALCULATION
+x2=x1*(exp((Eg/(2*kb))*((1/T1)-(1/T2))))//The ratio of conductiveness
+
+//OUTPUT
+printf('The conductivity of Ge at T2 is %3.4f ohm^-1 m^-1',x2)
diff --git a/1931/CH10/EX10.11/11.sce b/1931/CH10/EX10.11/11.sce new file mode 100755 index 000000000..2f7194aa4 --- /dev/null +++ b/1931/CH10/EX10.11/11.sce @@ -0,0 +1,15 @@ +clc
+clear
+//INPUT DATA
+Eg1=0.36//The energy gap of intrinsic semiconductor A in eV
+Eg2=0.72//The energy gap of intrinsic semiconductor B in eV
+T1=300//Temperature of semiconductor A in K
+T2=300//Temperature of semiconductor B in K
+m=9.11*10^-31//mass of an electron in Kg
+KT=0.026//kt in eV
+
+//CALCULATION
+x=(exp((Eg2-Eg1)/(2*KT)))//The intrinsic carrier density of A to B
+
+//OUTPUT
+printf('The intrinsic carrier density of A to B is %i',x)
diff --git a/1931/CH10/EX10.12/12.sce b/1931/CH10/EX10.12/12.sce new file mode 100755 index 000000000..13fb0be9b --- /dev/null +++ b/1931/CH10/EX10.12/12.sce @@ -0,0 +1,15 @@ +clc
+clear
+//INPUT DATA
+T1=293//Temperature in K
+T2=373//Temperature in K
+x1=250//The conductivity of semiconductor at T1 in ohm^-1 m^-1
+x2=1100//The conductivity of semiconductor at T2 in ohm^-1 m^-1
+e=1.6*10^-19//charge of electron in coulombs
+kb=1.38*10^-23//Boltzmann's constant m^2 Kg s^-2 k^-1
+
+//CALCULATION
+Eg=(2*kb*log(x2/x1)*((T1*T2)/(T2-T1)))/10^-20//The band gap of semiconductor in J*10^-20
+
+//OUTPUT
+printf('The band gap of semiconductor is %3.4f*10^-20 J',Eg)
diff --git a/1931/CH10/EX10.13/13.sce b/1931/CH10/EX10.13/13.sce new file mode 100755 index 000000000..781af8571 --- /dev/null +++ b/1931/CH10/EX10.13/13.sce @@ -0,0 +1,12 @@ +clc
+clear
+//INPUT DATA
+me=50//The electron mobility of pure semi conductor in m^2 V^-1 s^-1
+t1=4.2//temp of pure semi conductor in k
+t2=300//temp in k
+
+//CALCULATION
+m=me*((t2^(-3/2))/(t1^(-3/2)))//mobility of pure semi conductor in m^2 V^-1 s^-1
+
+//OUTPUT
+printf('mobility of pure semi conductor is %3.6f m^2 V^-1 s^-1',m)
diff --git a/1931/CH10/EX10.14/14.sce b/1931/CH10/EX10.14/14.sce new file mode 100755 index 000000000..9f791cbd1 --- /dev/null +++ b/1931/CH10/EX10.14/14.sce @@ -0,0 +1,14 @@ +clc
+clear
+//INPUT DATA
+ec1=19.96//The electrical conductivity of an intrinsic semi conductor in ohm^-1 m^-1
+ec2=79.44//The increasing electrical conductivity of an intrinsic semi conductor in ohm^-1 m^-1
+t1=333//temperature of an intrinsic semi conductor in k
+t2=373//increasing temperature of an intrinsic semi conductor in k
+kb=1.38*10^-23//Boltzmann's constant in m^2 Kg s^-2 k^-1
+
+//CALCULATION
+Eg=(2*kb*(log(ec2/ec1))*((t1*t2)/(t2-t1)))/10^-19//The band gap of an intrinsic semi conductor in J*10^-19
+
+//OUTPUT
+printf('The band gap of an intrinsic semi conductor is %3.6f*10^-19 J',Eg)
diff --git a/1931/CH10/EX10.2/2.sce b/1931/CH10/EX10.2/2.sce new file mode 100755 index 000000000..93a407361 --- /dev/null +++ b/1931/CH10/EX10.2/2.sce @@ -0,0 +1,13 @@ +clc
+clear
+//INPUT DATA
+d=2.37*10^19//The intrinsic carrier density at room temperature in m^-3
+me=0.38//The electron mobility in m^2 V^-1 s^-1
+mh=0.18//The hole mobility in m^2 V^-1 s^-1
+e=1.6*10^-19//charge of electron in coulombs
+
+//CALCULATION
+r=(1/(d*e*(me+mh)))//The resistivity of intrinsic carrier in ohm m
+
+//OUTPUT
+printf('The resistivity of intrinsic carrier is %3.4f ohm m',r)
diff --git a/1931/CH10/EX10.3/3.sce b/1931/CH10/EX10.3/3.sce new file mode 100755 index 000000000..0a0a7ddf2 --- /dev/null +++ b/1931/CH10/EX10.3/3.sce @@ -0,0 +1,13 @@ +clc
+clear
+//INPUT DATA
+r=2*10^-4//the resistivity of In-Sb in ohm m
+me=6//The electron mobility in m^2 V^-1 s^-1
+mh=0.2//The hole mobility in m^2 V^-1 s^-1
+e=1.6*10^-19//charge of electron in coulombs
+
+//CALCULATION
+d=(1/(r*e*(me+mh)))/10^21//The intrinsic carrier density at room tepmerature in m^-3 *10^21
+
+//OUTPUT
+printf('The intrinsic carrier density at room tepmerature is %3.3f *10^21 m^-3',d)
diff --git a/1931/CH10/EX10.4/4.sce b/1931/CH10/EX10.4/4.sce new file mode 100755 index 000000000..372deb7aa --- /dev/null +++ b/1931/CH10/EX10.4/4.sce @@ -0,0 +1,18 @@ +clc
+clear
+//INPUT DATA
+Eg=1.1*1.6*10^-19//The energy gap of silicon in J
+me=0.48//The electron mobility in m^2 V^-1 s^-1
+mh=0.13//The hole mobility in m^2 V^-1 s^-1
+h=6.625*10^-34//Planck's constant in m^2 Kg /sec
+e=1.6*10^-19//charge of electron in coulombs
+m=9.11*10^-31//mass of an electron
+kb=1.38*10^-23//Boltzmann's constant m^2 Kg s^-2 k^-1
+t=300//temperature in k
+
+//CALCULATION
+ni=2*((2*3.14*m*kb*t)/h^2)^(3/2)*exp(-Eg/(2*kb*t))//intrinsic carrier concentration in m^-3
+ec=(ni*e*(me+mh))/10^-3//The electrical conductivity at room temperature in ohm^-1 m^-1 *10^-3
+
+//OUTPUT
+printf('The electrical conductivity at room temperature is %3.4f *10^-3 ohm^-1 m^-1',ec)
diff --git a/1931/CH10/EX10.5/5.sce b/1931/CH10/EX10.5/5.sce new file mode 100755 index 000000000..1359ff5a7 --- /dev/null +++ b/1931/CH10/EX10.5/5.sce @@ -0,0 +1,20 @@ +clc
+clear
+//INPUT DATA
+Eg=1.43*1.6*10^-19//The energy gap of intrinsic GaAs in J
+xe=0.85//The electron mobility in m^2 V^-1 s^-1
+xh=0.04//The hole mobility in m^2 V^-1 s^-1
+me=0.068*9.11*10^-31//effective mass of electron in m
+mh=0.5*9.11*10^-31//effective mass of hole in m
+h=6.625*10^-34//Planck's constant in m^2 Kg /sec
+e=1.6*10^-19//charge of electron in coulombs
+m=9.11*10^-31//mass of an electron in Kg
+kb=1.38*10^-23//Boltzmann's constant m^2 Kg s^-2 k^-1
+t=300//temperature in k
+
+//CALCULATION
+ni=(2*((2*3.14*kb*t)/h^2)^(3/2)*(me*mh)^(3/4)*exp(-Eg/(2*kb*t)))/10^12//intrinsic carrier concentration in m^-3*10^12
+ec=(ni*10^12*e*(xe+xh))/10^-7//The electrical conductivity at room temperature in ohm^-1 m^-1 *10^-7
+
+//OUTPUT
+printf('The intrinsic carrier concentration is %3.4f*10^12 m^-3 \n The electrical conductivity at room temperature is %3.4f *10^-7 ohm^-1 m^-1',ni,ec)
diff --git a/1931/CH10/EX10.6/6.sce b/1931/CH10/EX10.6/6.sce new file mode 100755 index 000000000..3687c3044 --- /dev/null +++ b/1931/CH10/EX10.6/6.sce @@ -0,0 +1,16 @@ +clc
+clear
+//INPUT DATA
+Eg=1.12*1.6*10^-19//Energy gap of Si semi conductor in J
+me=0.12*9.11*10^-31//The electron mobility in m^2 V^-1 s^-1
+mh=0.28*9.11*10^-31//The hole mobility in m^2 V^-1 s^-1
+t=300//temperature of fermi level in k
+kb=1.38*10^-23//Boltzmann's constant m^2 Kg s^-2 k^-1
+m=9.11*10^-31//mass of an electron in Kg
+
+//CALCULATION
+Ef=((Eg/2)+(((3*kb*t)/4)*log(mh/me)))/10^-20//position of the fermi level in J *10^-20
+
+//OUTPUT
+printf('The position of the fermi level is %3.5f*10^-20 J',Ef)
+
diff --git a/1931/CH10/EX10.7/7.sce b/1931/CH10/EX10.7/7.sce new file mode 100755 index 000000000..0418f185a --- /dev/null +++ b/1931/CH10/EX10.7/7.sce @@ -0,0 +1,15 @@ +clc
+clear
+//INPUT DATA
+Eg=1*1.6*10^-19//Energy gap in J
+E=0.1*1.6*10^-19//Fermi level is shifted by 10% in J
+me=1*9.11*10^-31//The electron mobility in m^2 V^-1 s^-1
+mh=4*9.11*10^-31//Effective mass of holes is 4 times that of electrons that is the hole mobility in m^2 V^-1 s^-1
+m=9.11*10^-31//mass of an electron in Kg
+kb=1.38*10^-23//Boltzmann's constant m^2 Kg s^-2 k^-1
+
+//CALCULATION
+T=(4*E)/(3*kb*log(4))//The Temperature of the fermi level shifted by 10% from the middle of the forbidden energy gap in K
+
+//OUTPUT
+printf('The Temperature of the fermi level shifted by 10percentage from the middle of the forbidden energy gap is %3.2f K',T)
diff --git a/1931/CH10/EX10.8/8.sce b/1931/CH10/EX10.8/8.sce new file mode 100755 index 000000000..91b5cc970 --- /dev/null +++ b/1931/CH10/EX10.8/8.sce @@ -0,0 +1,19 @@ +clc
+clear
+//INPUT DATA
+l=1*10^-2//length of the intrinsic Ge rod in m
+b=1*10^-3//breadth of the intrinsic Ge rod in m
+t=1*10^-3//thickness of the intrinsic Ge rod in m
+T=300//temperature of the intrinsic Ge rod in K
+me=0.39//The electron mobility in m^2 V^-1 s^-1
+mh=0.19//The hole mobility in m^2 V^-1 s^-1
+ni=2.5*10^19//intrinsic carrier conduction in m^3
+e=1.6*10^-19//charge of electron in coulombs
+
+//CALCULATION
+ec=(ni*e*(me+mh))//The electrical conductivity at room temperature in ohm^-1 m^-1
+A=(b*t)//area in m^2
+R=(l/(ec*A))//The resistance of an intrinsic Ge rod in ohm
+
+//OUTPUT
+printf('The resistance of an intrinsic Ge rod is %i ohm',R)
diff --git a/1931/CH10/EX10.9/9.sce b/1931/CH10/EX10.9/9.sce new file mode 100755 index 000000000..b5fe1d0d5 --- /dev/null +++ b/1931/CH10/EX10.9/9.sce @@ -0,0 +1,14 @@ +clc
+clear
+//INPUT DATA
+Eg=1.2*1.6*10^-19//The energy gap of intrinsic semiconductor in J
+T1=600//Temperature in K
+T2=300//Temperature in K
+e=1.6*10^-19//charge of electron in coulombs
+kb=1.38*10^-23//Boltzmann's constant m^2 Kg s^-2 k^-1
+
+//CALCULATION
+x=exp((-Eg/(2*kb))*((1/T1)-(1/T2)))/10^5//The ratio of conductiveness*10^5
+
+//OUTPUT
+printf('The ratio of conductiveness is %3.2f*10^5',x)
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