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author | Thomas Stephen Lee | 2015-08-28 16:53:23 +0530 |
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committer | Thomas Stephen Lee | 2015-08-28 16:53:23 +0530 |
commit | 4a1f703f1c1808d390ebf80e80659fe161f69fab (patch) | |
tree | 31b43ae8895599f2d13cf19395d84164463615d9 /Materials_Science_by_Dr._M._Arumugam/Chapter4.ipynb | |
parent | 9d260e6fae7328d816a514130b691fbd0e9ef81d (diff) | |
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diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter4.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter4.ipynb new file mode 100755 index 00000000..8da77cca --- /dev/null +++ b/Materials_Science_by_Dr._M._Arumugam/Chapter4.ipynb @@ -0,0 +1,370 @@ +{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "#4: Electron Theory of Solids"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.1, Page number 4.57"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 10,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "de broglie wavelength is 0.00286 angstrom\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "E=10**4*1.6*10**-19; #kinetic energy(J)\n",
+ "m=1.675*10**-27; #mass(kg)\n",
+ "h=6.625*10**-34; #planck's constant\n",
+ "\n",
+ "#Calculation\n",
+ "v=math.sqrt(2*E/m); #velocity(m/s)\n",
+ "lamda=h/(m*v); #de broglie wavelength(m)\n",
+ "\n",
+ "#Result\n",
+ "print \"de broglie wavelength is\",round(lamda*10**10,5),\"angstrom\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.2, Page number 4.58"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 11,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "energy difference is 1.81 *10**-37 J\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "m=9.1*10**-31; #mass(kg)\n",
+ "nx=ny=nz=1;\n",
+ "n=6;\n",
+ "a=1; #edge(m)\n",
+ "h=6.63*10**-34; #planck's constant\n",
+ "\n",
+ "#Calculation\n",
+ "E1=h**2*(nx**2+ny**2+nz**2)/(8*m*a**2);\n",
+ "E2=h**2*n/(8*m*a**2);\n",
+ "E=E2-E1; #energy difference(J)\n",
+ "\n",
+ "#Result\n",
+ "print \"energy difference is\",round(E*10**37,2),\"*10**-37 J\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.3, Page number 4.58"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 15,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "temperature is 1261 K\n",
+ "answer varies due to rounding off errors\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "y=1/100; #percentage of probability\n",
+ "x=0.5*1.6*10**-19; #energy(J)\n",
+ "k=1.38*10**-23; #boltzmann constant\n",
+ "\n",
+ "#Calculation\n",
+ "xbykT=math.log((1/y)-1);\n",
+ "T=x/(k*xbykT); #temperature(K)\n",
+ "\n",
+ "#Result\n",
+ "print \"temperature is\",int(T),\"K\"\n",
+ "print \"answer varies due to rounding off errors\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.4, Page number 4.58"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 16,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "fermi energy is 3.15 eV\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "d=970; #density(kg/m**3)\n",
+ "Na=6.02*10**26; #avagadro number\n",
+ "w=23; #atomic weight\n",
+ "m=9.1*10**-31; #mass(kg)\n",
+ "h=6.62*10**-34; #planck's constant\n",
+ "\n",
+ "#Calculation\n",
+ "N=d*Na/w; #number of atoms/m**3\n",
+ "x=h**2/(8*m);\n",
+ "y=(3*N/math.pi)**(2/3);\n",
+ "EF=x*y; #fermi energy(J)\n",
+ "\n",
+ "#Result\n",
+ "print \"fermi energy is\",round(EF/(1.6*10**-19),2),\"eV\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.5, Page number 4.59"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 18,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "work function is 4.14 eV\n",
+ "maximum kinetic energy is 0.758 eV\n",
+ "answer varies due to rounding off errors\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "h=6.625*10**-34; #planck's constant\n",
+ "c=3*10**8; #velocity of light(m/s)\n",
+ "lamda0=3000*10**-10; #wavelength(m)\n",
+ "e=1.6*10**-19; #charge(coulomb)\n",
+ "lamda=2536*10**-10; #wavelength(m)\n",
+ "\n",
+ "#Calculation\n",
+ "hf0=c*h/(lamda0*e); #work function(eV)\n",
+ "E=c*h*((1/lamda)-(1/lamda0))/e; #maximum kinetic energy(eV)\n",
+ "\n",
+ "#Result\n",
+ "print \"work function is\",round(hf0,2),\"eV\"\n",
+ "print \"maximum kinetic energy is\",round(E,3),\"eV\"\n",
+ "print \"answer varies due to rounding off errors\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.6, Page number 4.59"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 19,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "lowest energy of neutron is 2.05 MeV\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "n=1;\n",
+ "hbar=1.054*10**-34; \n",
+ "m=1.67*10**-27; #mass of neutron(kg)\n",
+ "a=10**-14; #size(m)\n",
+ "\n",
+ "#Calculation\n",
+ "E=n**2*math.pi**2*hbar**2/(2*m*a**2); #lowest energy of neutron(J)\n",
+ "\n",
+ "#Result\n",
+ "print \"lowest energy of neutron is\",round(E/(1.6*10**-13),2),\"MeV\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.7, Page number 4.59"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 20,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "probability of particle is 0.0158\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "from scipy.integrate import quad\n",
+ "\n",
+ "#Variable declaration\n",
+ "k=1;\n",
+ "\n",
+ "#Calculation\n",
+ "def zintg(x):\n",
+ "\treturn math.exp(-2*k*x)\n",
+ "\n",
+ "a=quad(zintg,2/k,3/k)[0]; #probability of particle\n",
+ "\n",
+ "#Result\n",
+ "print \"probability of particle is\",round(2*a,4)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 4.8, Page number 4.60"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 22,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "voltage appeared is 1.83 mV\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "i=10**-2; #current(ampere)\n",
+ "A=0.01*0.001; #area(m**2)\n",
+ "RH=3.66*10**-4; #hall coefficient(m**3/coulomb)\n",
+ "Bz=0.5; #magnetic induction(weber/m**2)\n",
+ "\n",
+ "#Calculation\n",
+ "Jx=i/A; \n",
+ "Ey=RH*Bz*Jx; \n",
+ "Vy=Ey*i; #voltage appeared(V)\n",
+ "\n",
+ "#Result\n",
+ "print \"voltage appeared is\",Vy*10**3,\"mV\""
+ ]
+ }
+ ],
+ "metadata": {
+ "kernelspec": {
+ "display_name": "Python 2",
+ "language": "python",
+ "name": "python2"
+ },
+ "language_info": {
+ "codemirror_mode": {
+ "name": "ipython",
+ "version": 2
+ },
+ "file_extension": ".py",
+ "mimetype": "text/x-python",
+ "name": "python",
+ "nbconvert_exporter": "python",
+ "pygments_lexer": "ipython2",
+ "version": "2.7.9"
+ }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 0
+}
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