{ "metadata": { "name": "" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Chapter 11:Nuclear Structure" ] }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example no:11.1,Page no:393" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Variable declaration \n", "u= 1.66*(10**(-27)) #atomic mass unit, kg\n", "Mc= 12*u # atomic mass of Carbon-12, kg\n", "R= 2.7 #radius of nucleus, fm\n", "\n", "#Calculation\n", "import math\n", "R=R*(10**(-15)) #converting to m\n", "density= Mc/((4.0/3.0)*(math.pi)*(R**3)) # kg/m**3\n", "\n", "#Calculation\n", "print\"Density of Carbon 12 nucleus is:%.2g\"%density,\"kg/m**3\"\n", " \n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Density of Carbon 12 nucleus is:2.4e+17 kg/m**3\n" ] } ], "prompt_number": 2 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example no:11.2,Page no:393" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Variable declaration\n", "r= 2.4 #distance between centre of the protons, fm\n", "r= r*(10**(-15)) #converting to m\n", "e= 1.6*(10**(-19)) #charge of an electron, C\n", "Po= 8.85*(10**(-12)) #Permittivity of free space, F/m\n", "\n", "#Calculation\n", "K=1/(4*(math.pi)*Po) #constant, N.m**2/C**2\n", "F= K*(e**2)/(r**2) #N\n", "\n", "#Result\n", "print\"The repulsive force is: \",round(F),\"N\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "The repulsive force is: 40.0 N\n" ] } ], "prompt_number": 3 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example no:11.3,Page no:395" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Variable declaration\n", "B= 1.0 #strength of magnetic field, T\n", "Mneutron= 3.152*(10**(-8)) #Magnetic moment for neutron, eV/T\n", "\n", "#Calculation\n", "#Part (a)\n", "Mproton= 2.793*Mneutron #Magnetic moment for proton, eV/T\n", "dE= 2*Mproton*B #eV\n", "#Part (b)\n", "h= 4.13*(10**(-15)) #Planck's constant, eV.s\n", "Flarmor= dE/h #Hz\n", "Flarmor= Flarmor/(10**6) #converting to MHz\n", "\n", "#Result\n", "print\"(a).The energy difference is:%.4g\"%dE,\"eV\"\n", "print\"(b).The Larmor frequency for a proton in the field is:\",round(Flarmor,1),\"MHz(APPROX)\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "(a).The energy difference is:1.761e-07 eV\n", "(b).The Larmor frequency for a proton in the field is: 42.6 MHz(APPROX)\n" ] } ], "prompt_number": 4 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example no:11.4,Page no:401" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Variable declaration \n", "Ebinding= 160.647 #binding nergy, MeV\n", "Mh= 1.007825 #Mass of H1 atom, u\n", "Mn= 1.008665 #Mass of neutron, u\n", "Z=10 #number of protons\n", "N=10 #number of neutrons\n", "\n", "#Calculation\n", "Mneon= ((Z*Mh)+(N*Mn))-(Ebinding/931.49) #using Eqn 11.7\n", "\n", "#Result\n", "print\"The atomic mass of Neon 10 isotope is: \",round(Mneon,3),\"u\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "The atomic mass of Neon 10 isotope is: 19.992 u\n" ] } ], "prompt_number": 5 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example no:11.5,Page no:402" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Variable declaration\n", "\n", "#Part(a)\n", "Ca_42=41.958622 #[u] Mass of 42Ca20 \n", "\n", "#from table\n", "M_neutron=1.008665 #[u] Mass of a free neutron\n", "Ca_41=40.962278 #[u] Mass of 41Ca20 after removal of 1 neutron\n", "#Part(b):\n", "#from table\n", "M_proton=1.007276466812 #[u] Mass of a free proton\n", "K_19=40.96237 #[u] Mass of Potasium Isotope 41K19\n", "\n", "\n", "#Calculation\n", "#Part (a):\n", "n_total=Ca_41+M_neutron\n", "p_total=K_19+M_proton\n", "neutron_BE=931.49*(n_total-Ca_42)#Binding energy in MeV\n", "proton_BE=931.49*(p_total-Ca_42)\n", "print \"(a).Binding energy of missing neutron is: \",round(neutron_BE,2),\"MeV\"\n", "print\"(b).Binding energy for missing proton=\",round(proton_BE,2),\"MeV\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "(a).Binding energy of missing neutron is: 11.48 MeV\n", "(b).Binding energy for missing proton= 10.27 MeV\n" ] } ], "prompt_number": 6 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example no:11.6,Page no:407" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Variable declaration \n", "Z= 30.0 #proton number\n", "N=34.0 #Neutron number\n", "\n", "#Calculation\n", "#Using Eqn 11.7\n", "Mh= 1.007825 #Mass of H1 atom, u\n", "Mn= 1.008665 #Mass of neutron, u\n", "Mzinc= 63.929 #atomic mass of zinc, u\n", "Ebinding= ((Z*Mh)+(N*Mn)-Mzinc)*931.49 #MeV\n", "#Using semiempirical formula, Eqn 11.18, Page 407\n", "a1= 14.1 #Mev\n", "a2= 13.0 #MeV\n", "a3= 0.595 #Mev\n", "a4= 19.0 #MeV\n", "a5= 33.5 #MeV\n", "A= Z+N \n", "E2= ((a1*A)-(a2*(A**(2.0/3.0)))-(a3*Z*(Z-1)/(A**(1.0/3.0)))-(a4*((A-2*Z)**2)/A)+(a5/(A**(3.0/4.0)))) #MeV\n", "\n", "#Result\n", "print\"Binding energy of Zinc 64 isotope is: \",round(Ebinding,1),\"MeV\"\n", "print\"The binding energy using semi-empirical formula, in MeV, is: \",round(E2,1),\"MeV\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Binding energy of Zinc 64 isotope is: 559.2 MeV\n", "The binding energy using semi-empirical formula, in MeV, is: 561.7 MeV\n" ] } ], "prompt_number": 7 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example no:11.7,Page no:408" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Variable declaration\n", "A=25\n", "\n", "#Calculation\n", "#Derivation part\n", "#dEb/dZ=-a3*(2*z-1)/A^(1/3)+4*a4*(A-2*Z)/A\n", "#Z=a3*A**-1/3+4*a4/(2*a3*A^-1/3+8*a4*A**-1)\n", "Z=(0.595*A**(-1.0/3.0)+76)/(1.19*A**(-1.0/3.0)+(152*A**-1))\n", "print \"For A=25,Z=\",round(Z,1),\"\\nfor which we conclude that Z=\",round(Z),\"should be the atomic no. of most stable isobar of A=25\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "For A=25,Z= 11.7 \n", "for which we conclude that Z= 12.0 should be the atomic no. of most stable isobar of A=25\n" ] } ], "prompt_number": 8 } ], "metadata": {} } ] }