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authorTrupti Kini2016-10-12 23:31:00 +0600
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A Applied_Physics_by_S._Mani_Naidu/Chapter1.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter10.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter11.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter13.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter2.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter3.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter4.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter5.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter6.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter7.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter8.ipynb A Applied_Physics_by_S._Mani_Naidu/Chapter9.ipynb A Applied_Physics_by_S._Mani_Naidu/screenshots/11.png A Applied_Physics_by_S._Mani_Naidu/screenshots/22.png A Applied_Physics_by_S._Mani_Naidu/screenshots/33.png A "sample_notebooks/ravindra m gowda/Chapter_1_Basics_of_thermodynamics_Rudramani.ipynb"
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+{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# 2: Crystal Structures"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example number 1, Page number 2-16"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 2,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "free volume per unit cell is 0.007675 nm**3\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "r=0.1249; #radius(nm)\n",
+ "n=2; #number of atoms\n",
+ "\n",
+ "#Calculation\n",
+ "a=4*r/math.sqrt(3); #unit cell edge length(nm)\n",
+ "V=a**3; #volume of unit cell(nm**3)\n",
+ "v=4*n*math.pi*r**3/3; #volume of atoms in unit cell(nm**3)\n",
+ "fv=V-v; #free volume per unit cell(nm**3)\n",
+ "\n",
+ "#Result\n",
+ "print \"free volume per unit cell is\",round(fv,6),\"nm**3\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example number 2, Page number 2-16"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 3,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "lattice constant is 3.517 angstrom\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "N=6.02*10**26; #Avagadro Number\n",
+ "n=2;\n",
+ "rho=530; #density(kg/m**3)\n",
+ "M=6.94; #atomic weight(amu)\n",
+ "\n",
+ "#Calculation\n",
+ "a=(n*M/(rho*N))**(1/3)*10**10; #lattice constant(angstrom)\n",
+ "\n",
+ "#Result\n",
+ "print \"lattice constant is\",round(a,3),\"angstrom\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example number 3, Page number 2-17"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 7,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "lattice constant is 2.87 angstrom\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "N=6.02*10**23; #Avagadro Number\n",
+ "n=2;\n",
+ "rho=7860; #density(kg/m**3)\n",
+ "M=55.85; #atomic weight(amu)\n",
+ "\n",
+ "#Calculation\n",
+ "a=(n*M/(rho*N))**(1/3)*10**9; #lattice constant(angstrom)\n",
+ "\n",
+ "#Result\n",
+ "print \"lattice constant is\",round(a,2),\"angstrom\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example number 4, Page number 2-17"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 9,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "number of atoms per m**3 is 177.3 *10**27 atoms/m**3\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "n=8; #number of atoms\n",
+ "a=0.356*10**-9; #lattice constant(m)\n",
+ "\n",
+ "#Calculation\n",
+ "N=n/a**3; #number of atoms per m**3\n",
+ " \n",
+ "#Result\n",
+ "print \"number of atoms per m**3 is\",round(N/10**27,1),\"*10**27 atoms/m**3\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example number 5, Page number 2-17"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 11,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "number of atoms per sq mm is 8.16 *10**12\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "a=3.5; #lattice constant(angstrom)\n",
+ "n=10**7; #1mm in angstrom\n",
+ "\n",
+ "#Calculation\n",
+ "N=n**2/a**2; #number of atoms per sq mm\n",
+ " \n",
+ "#Result\n",
+ "print \"number of atoms per sq mm is\",round(N/10**12,2),\"*10**12\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example number 6, Page number 2-18"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 13,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "density is 5434.5 kg/m**3\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "N=6.02*10**26; #Avagadro Number\n",
+ "n=8; #number of atoms\n",
+ "a=5.62*10**-10; #lattice constant(m)\n",
+ "M=72.59; #atomic weight(amu)\n",
+ "\n",
+ "#Calculation\n",
+ "rho=n*M/(a**3*N); #density(kg/m**3)\n",
+ " \n",
+ "#Result\n",
+ "print \"density is\",round(rho,1),\"kg/m**3\""
+ ]
+ }
+ ],
+ "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": "2.7.11"
+ }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 0
+}