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author | Trupti Kini | 2016-10-20 23:30:55 +0600 |
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committer | Trupti Kini | 2016-10-20 23:30:55 +0600 |
commit | 1146bfed5bd1d9b56e8e91a6c3a7160fc006bc70 (patch) | |
tree | baad6e907a57b4e9ddf32bc5a1baeca7666ed69d /sample_notebooks | |
parent | e5ca7d9515ea0c72b50e9d67b31896cf83e1e318 (diff) | |
download | Python-Textbook-Companions-1146bfed5bd1d9b56e8e91a6c3a7160fc006bc70.tar.gz Python-Textbook-Companions-1146bfed5bd1d9b56e8e91a6c3a7160fc006bc70.tar.bz2 Python-Textbook-Companions-1146bfed5bd1d9b56e8e91a6c3a7160fc006bc70.zip |
Added(A)/Deleted(D) following books
A Engineering_Mechanics_by_A._K._Tayal/Chapter_10_UNIFORM_FLEXIBLE_SUSPENSION_CABLES.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_12_MOMENT_OF_INERTIA.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_13_PRINCIPLE_OF_VIRTUAL_WORK.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_14_RECTILINEAR_MOTION_OF_A_PARTICLE.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_15_CURVILINEAR_MOTION_OF_A_PARTICLE.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_16_KINETICS_OF_A_PARTICLE_WORK_AND_ENERGY_.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_17_KINETICS_OF_PARTICLE_IMPULSE_AND_MOMENTUM.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_18___IMPACT_COLLISION_OF_ELASTIC_BODIES.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_19_RELATIVE_MOTION.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_20_MOTION_OF_PROJECTILE.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_21_KINEMATICS_OF_RIGID_BODY.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_22_KINETICS_OF_RIGID_BODY_FORCE_AND_ACCELERATION.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_23_KINETICS_OF_RIGID_BODY_WORK_AND_ENERGY.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_24_MECHANICAL_VIBRATIONS.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_25_____SHEAR_FORCE_AND_BENDING_MOMENT.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_26_APPENDIX.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_2_CONCURRENT_FORCES_IN_A_PLANE.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_3_PARALLEL_FORCES_IN_A_PLANE.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_4_CENTROID_CENTRE_OF_MASS_AND_CENTRE_OF_GRAVITY.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_5__GENERAL_CASE_OF_FORCES_IN_A_PLANE.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_6_FRICTION.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_7_APPLICATION_OF_FRICTION.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_8______SIMPLE_LIFTING_MACHINES.ipynb
A Engineering_Mechanics_by_A._K._Tayal/Chapter_9_ANALYSIS_OF_PLANE_TRUSSES_AND_FRAMES.ipynb
A Engineering_Mechanics_by_A._K._Tayal/screenshots/10.4.png
A Engineering_Mechanics_by_A._K._Tayal/screenshots/12.7.png
A Engineering_Mechanics_by_A._K._Tayal/screenshots/13.7.png
A sample_notebooks/ajinkyakhair/chapter2_8f8MyfH.ipynb
Diffstat (limited to 'sample_notebooks')
-rw-r--r-- | sample_notebooks/ajinkyakhair/chapter2_8f8MyfH.ipynb | 337 |
1 files changed, 337 insertions, 0 deletions
diff --git a/sample_notebooks/ajinkyakhair/chapter2_8f8MyfH.ipynb b/sample_notebooks/ajinkyakhair/chapter2_8f8MyfH.ipynb new file mode 100644 index 00000000..5bd122ad --- /dev/null +++ b/sample_notebooks/ajinkyakhair/chapter2_8f8MyfH.ipynb @@ -0,0 +1,337 @@ +{ + "metadata": { + "name": "", + "signature": "sha256:74a00fabf3de3a229499fd336c46d9a546ea42ad7cb4fbe98a92a6ea72f21fa8" + }, + "nbformat": 3, + "nbformat_minor": 0, + "worksheets": [ + { + "cells": [ + { + "cell_type": "heading", + "level": 1, + "metadata": {}, + "source": [ + "Chapter 2: Bonding in Solids" + ] + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.1,Page number 62" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "epsilon_0 = 8.854*10**-12; # Absolute electrical permittivity of free space, F/m\n", + "e = 1.6*10**-19; # Energy equivalent of 1 eV, eV/J\n", + "r = 3.147*10**-10; # Nearest neighbour distance for KCl, m\n", + "n = 9.1; # Repulsive exponent of KCl\n", + "A = 1.748; # Madelung constant for lattice binding energy\n", + "E = A*e**2/(4*math.pi*epsilon_0*r)*(n-1)/n/e; # Binding energy of KCl, eV\n", + "print\"The binding energy of KCl = \",round(E,4),\"eV\";\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The binding energy of KCl = 7.10982502818 eV\n" + ] + } + ], + "prompt_number": 5 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.2,Page number 62" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "\n", + "epsilon_0 = 8.854*10**-12; # Absolute electrical permittivity of free space, F/m\n", + "N = 6.023*10**23; # Avogadro's number\n", + "e = 1.6*10**-19; # Energy equivalent of 1 eV, eV/J\n", + "a0 = 5.63*10**-10; # Lattice parameter of NaCl, m\n", + "r0 = a0/2; # Nearest neighbour distance for NaCl, m\n", + "n = 8.4; # Repulsive exponent of NaCl\n", + "A = 1.748; # Madelung constant for lattice binding energy\n", + "E = A*e**2/(4*pi*epsilon_0*r0)*(n-1)/n/e; # Binding energy of NaCl, eV\n", + "print\"The binding energy of NaCl = \",round(E*N*e/(4.186*1000),4),\"kcal/mol\" ;\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The binding energy of NaCl = 181.1005 kcal/mol\n" + ] + } + ], + "prompt_number": 7 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.3,Page number 62" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "\n", + "epsilon_0 = 8.854*10**-12; # Absolute electrical permittivity of free space, F/m\n", + "N = 6.023*10**23; # Avogadro's number\n", + "e = 1.6*10**-19; # Energy equivalent of 1 eV, eV/J\n", + "E = 162.9*10**3; # Binding energy of KCl, cal/mol\n", + "n = 8.6; # Repulsive exponent of KCl\n", + "A = 1.747; # Madelung constant for lattice binding energy\n", + "# As lattice binding energy, E = A*e**2/(4*%pi*epsilon_0*r0)*(n-1)/n, solving for r0\n", + "r0 = A*N*e**2/(4*pi*epsilon_0*E*4.186)*(n-1)/n; # Nearest neighbour distance of KCl, m\n", + "print\"The nearest neighbour distance of KCl = \",round(r0*10**10,4),\"angstorm\";\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The nearest neighbour distance of KCl = 3.1376 angstorm\n" + ] + } + ], + "prompt_number": 12 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.4,Page number 63" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "\n", + "epsilon_0 = 8.854*10**-12; # Absolute electrical permittivity of free space, F/m\n", + "N = 6.023*10**23; # Avogadro's number\n", + "e = 1.6*10**-19; # Energy equivalent of 1 eV, eV/J\n", + "E = 152*10**3; # Binding energy of CsCl, cal/mol\n", + "n = 10.6; # Repulsive exponent of CsCl\n", + "A = 1.763; # Madelung constant for lattice binding energy\n", + "\n", + "# As lattice binding energy, E = A*e**2/(4*pi*epsilon_0*r0)*(n-1)/n, solving for r0\n", + "r0 = A*N*e**2/(4*pi*epsilon_0*E*4.186)*(n-1)/n; # Nearest neighbour distance of CsCl, m\n", + "print\"The nearest neighbour distance of CsCl = \",round(r0*10**10,4),\"angstrom\";\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The nearest neighbour distance of CsCl = 3.4776 angstrom\n" + ] + } + ], + "prompt_number": 13 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.5,Page number 63" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "\n", + "epsilon_0 = 8.854*10**-12; # Absolute electrical permittivity of free space, F/m\n", + "N = 6.023*10**23; # Avogadro's number\n", + "e = 1.6*10**-19; # Energy equivalent of 1 eV, eV/J\n", + "r0 = 6.46*10**-10; # Nearest neighbour distance of NaI\n", + "E = 157.1*10**3; # Binding energy of NaI, cal/mol\n", + "A = 1.747; # Madelung constant for lattice binding energy\n", + "\n", + "# As lattice binding energy, E = -A*e**2/(4*pi*epsilon_0*r0)*(n-1)/n, solving for n\n", + "n = 1/(1+(4.186*E*4*pi*epsilon_0*r0)/(N*A*e**2)); # Repulsive exponent of NaI\n", + "print\"\\nThe repulsive exponent of NaI = \",round(n,4);" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "\n", + "The repulsive exponent of NaI = 0.363\n" + ] + } + ], + "prompt_number": 15 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.6,Page number 63" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "\n", + "e = 1.6*10**-19; # Energy equivalent of 1 eV, eV/J\n", + "a0 = 2.8158*10**-10; # Nearest neighbour distance of solid\n", + "A = 1.747; # Madelung constant for lattice binding energy\n", + "n = 8.6; # The repulsive exponent of solid\n", + "c = 2; # Structural factor for rocksalt\n", + "# As n = 1 + (9*c*a0**4)/(K0*e**2*A), solving for K0\n", + "K0 = 9*c*a0**4/((n-1)*e**2*A); # Compressibility of solid, metre square per newton\n", + "print\"The compressibility of the solid = \", \"{0:.3e}\".format(K0),\"metre square per newton\";" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The compressibility of the solid = 3.329e-01 metre square per newton\n" + ] + } + ], + "prompt_number": 18 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.7,Page number 69" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "\n", + "chi_diff = 1; # Electronegativity difference between the constituent of elements of solid\n", + "percent_ion = 100*(1-math.e**(-(0.25*chi_diff**2))); # Percentage ionic character present in solid given by Pauling\n", + "print\"The percentage ionic character present in solid = \",round(percent_ion,2),\"percent \";\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The percentage ionic character present in solid = 22.12 percent \n" + ] + } + ], + "prompt_number": 20 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 2.8,Page number 69" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "\n", + "#Given Data\n", + "\n", + "Eh_GaAs = 4.3; # Homopolar gap of GaAs compound, eV\n", + "C_GaAs = 2.90; # Ionic gap of GaAs compound, eV\n", + "Eh_CdTe = 3.08; # Homopolar gap of CdTe compound, eV\n", + "C_CdTe = 4.90; # Ionic gap of CdTe compound, eV\n", + "\n", + "fi_GaAs = C_GaAs**2/(Eh_GaAs**2 + C_GaAs**2);\n", + "fi_CdTe = C_CdTe**2/(Eh_CdTe**2 + C_CdTe**2);\n", + "print\"The fractional ionicity of GaAs = \",round(fi_GaAs,4);\n", + "print\"The fractional ionicity of CdTe = \",round(fi_CdTe,4);\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The fractional ionicity of GaAs = 0.3126\n", + "The fractional ionicity of CdTe = 0.7168\n" + ] + } + ], + "prompt_number": 3 + }, + { + "cell_type": "code", + "collapsed": false, + "input": [], + "language": "python", + "metadata": {}, + "outputs": [] + } + ], + "metadata": {} + } + ] +}
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