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| author | Trupti Kini | 2016-07-27 23:30:30 +0600 |
|---|---|---|
| committer | Trupti Kini | 2016-07-27 23:30:30 +0600 |
| commit | 72a8809fba69879b5a1733adab3d9ce4e79ff369 (patch) | |
| tree | f94ba99f588847f2dfbdc8e352091956b5632f5c /sample_notebooks/pratiksonone/Chapter1_1.ipynb | |
| parent | 33c8c0a7f0fef7bfe22cbc68c215549d003012be (diff) | |
| download | Python-Textbook-Companions-72a8809fba69879b5a1733adab3d9ce4e79ff369.tar.gz Python-Textbook-Companions-72a8809fba69879b5a1733adab3d9ce4e79ff369.tar.bz2 Python-Textbook-Companions-72a8809fba69879b5a1733adab3d9ce4e79ff369.zip | |
Added(A)/Deleted(D) following books
A "sample_notebooks/Reshma Ustad/Chapter_2_Properties_Of_Material.ipynb"
A sample_notebooks/kartiksankhla/Chapter2_1.ipynb
A sample_notebooks/pratiksonone/Chapter1_1.ipynb
Diffstat (limited to 'sample_notebooks/pratiksonone/Chapter1_1.ipynb')
| -rw-r--r-- | sample_notebooks/pratiksonone/Chapter1_1.ipynb | 710 |
1 files changed, 710 insertions, 0 deletions
diff --git a/sample_notebooks/pratiksonone/Chapter1_1.ipynb b/sample_notebooks/pratiksonone/Chapter1_1.ipynb new file mode 100644 index 00000000..e45e4d58 --- /dev/null +++ b/sample_notebooks/pratiksonone/Chapter1_1.ipynb @@ -0,0 +1,710 @@ +{
+ "metadata": {
+ "name": "",
+ "signature": "sha256:3cf7334f303e62e9d7ee028942cc3f913423a0b853c51242dbc7d672a0097072"
+ },
+ "nbformat": 3,
+ "nbformat_minor": 0,
+ "worksheets": [
+ {
+ "cells": [
+ {
+ "cell_type": "heading",
+ "level": 1,
+ "metadata": {},
+ "source": [
+ "Chapter1-General properties of Atomic Nucleus"
+ ]
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex1-pg51"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "##Exa1.1 : : Page 51 (2011)\n",
+ "#calculate distance of closet apporach\n",
+ "Z = 79.; ## Atomic number of Gold \n",
+ "z = 1.; ## Atomic number of Hydrogen\n",
+ "e = 1.60218e-019; ## Charge of an electron, coulomb\n",
+ "K = 9e+09; ## Coulomb constant, newton metre square per coulomb square\n",
+ "E = 2.*1.60218e-013; ## Energy of the proton, joule\n",
+ "b = Z*z*e**2.*K/E; ## Distance of closest approach, metre\n",
+ "print'%s %.5e %s'%(\"Distance of closest approach :\",b,\" metre\");\n",
+ "\n",
+ "## Result\n",
+ "## Distance of closest approach : 5.69575e-014 meter \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Distance of closest approach : 5.69575e-14 metre\n"
+ ]
+ }
+ ],
+ "prompt_number": 1
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex2-pg51"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Page 51 (2011)\n",
+ "import math\n",
+ "A = 14.; ## Number of protons\n",
+ "Z = 7.; ## Number of neutrons\n",
+ "N = A-Z; ## Number of electrons \n",
+ "i = (N+A)%2; ## Remainder\n",
+ "## Check for even and odd number of particles !!!!! \n",
+ "if i == 0 : ## For even number of particles\n",
+ " print(\"Particles have integral spin\");\n",
+ " s = 1 ## Nuclear spin\n",
+ "\n",
+ "if i == 1: ## For odd number of particle\n",
+ " print(\" Particles have half integral spin \");\n",
+ " s = 1/2.\n",
+ "\n",
+ "if s == 1 :\n",
+ " print( \"Measured value agree with the assumption\");\n",
+ "\n",
+ "if s == 1/2. :\n",
+ " print(\"Measured value disagree with the assumption\" );\n",
+ "\n",
+ "\n",
+ "## Result\n",
+ "## Particles have half integral spin \n",
+ "## Measured value disagree with the assumption \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ " Particles have half integral spin \n",
+ "Measured value disagree with the assumption\n"
+ ]
+ }
+ ],
+ "prompt_number": 2
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex3-pg52"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.3 : : Page 52 (2011)\n",
+ "import math\n",
+ "p = 62.; ## Momentum of the electron, MeV/c\n",
+ "K = 9e+09; ## Coulomb constant\n",
+ "E = 0.511; ## Energy of the electron, MeV\n",
+ "e = 1.60218e-019; ## Charge of an electron, C\n",
+ "Z = 23.; ## Atomic number\n",
+ "R = 0.5*10**-14; ## Diameter of the nucleus, meter\n",
+ "T = math.sqrt(p**2+E**2.)-E; ## Kinetic energy of the electron,MeV\n",
+ "E_c = -Z*K*e**2./(R*1.60218e-013); ## Coulomb energy, MeV\n",
+ "print'%s %.1f %s %.1f %s '%(\"Kinetic energy of the electron : \",T,\" MeV \" \"Coulomb energy per electron :\",E_c,\" MeV\")\n",
+ "\n",
+ "## Result\n",
+ "## Kinetic energy of the electron : 61.49 MeV \n",
+ "## Coulomb energy per electron : -6.633 MeV \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Kinetic energy of the electron : 61.5 MeV Coulomb energy per electron : -6.6 MeV \n"
+ ]
+ }
+ ],
+ "prompt_number": 6
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex4-pg52"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.4 : : Page 52 (2011) \n",
+ "import math\n",
+ "K = 500.*1.60218e-013; ## Kinetic energy of the electron,joule\n",
+ "h = 6.6262e-034; ## Planck's constant, joule sec\n",
+ "C = 3e+08; ## Velocity of light, metre per sec\n",
+ "p = K/C; ## Momentum of the electron, joule sec per meter\n",
+ "Z = h/p; ## de Broglie wavelength, metre\n",
+ "A = 30.*math.pi/180.; ## Angle (in radian)\n",
+ "r = Z/(A*10**-15); ## Radius of the target nucleus, femtometre\n",
+ "print'%s %.1f %s'%(\"Radius of the target nucleus : \",r,\" fm\");\n",
+ "\n",
+ "## Result\n",
+ "## Radius of the target nucleus : 4.74 fm\n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Radius of the target nucleus : 4.7 fm\n"
+ ]
+ }
+ ],
+ "prompt_number": 7
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex5-pg52"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.5 : : Page 52 (2011) \n",
+ "import math\n",
+ "#calculate radius of the nucleus\n",
+ "e = 1.60218e-019; ## Charge of an electron, C\n",
+ "A = 33.; ## Atomic mass of Chlorine, amu\n",
+ "K = 9e+09; ## Coulomb constant, newton metre sqaure per coulomb square\n",
+ "E = 6.1*1.60218e-013; ## Coulomb energy, joule\n",
+ "R_0 = 3./5.*K/E*e**2.*(A)**(2./3.); ## Distance of closest approach, metre\n",
+ "R = R_0*A**(1./3.); ## Radius of the nucleus, metre\n",
+ "print'%s %.2e %s'%(\"Radius of the nucleus : \",R,\"metre\");\n",
+ "\n",
+ "## Result\n",
+ "## Radius of the nucleus : 4.6805e-015 metre \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Radius of the nucleus : 4.68e-15 metre\n"
+ ]
+ }
+ ],
+ "prompt_number": 8
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex6-pg53"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.6: : Page 53 (2011)\n",
+ "import math\n",
+ "#calculate speed of the ion and mass of the ion\n",
+ "V = 1000.; ## Potential difference, volts\n",
+ "R = 18.2e-02; ## Radius of the orbit, metre\n",
+ "B = 1000e-04; ## Magnetic field, tesla\n",
+ "e = 1.60218e-019; ## Charge of an electron, C\n",
+ "n = 1.; ## Number of the ion\n",
+ "v = 2.*V/(R*B); ## Speed of the ion, metre per sec\n",
+ "M = 2.*n*e*V/v**2.; ## Mass of the ion, Kg\n",
+ "print'%s %.4e %s %.1f %s '%(\"Speed of the ion: \",v,\" m/s \"\"Mass of the ion : \", M/1.67e-027,\" u\");\n",
+ "\n",
+ "## Result\n",
+ "## Speed of the ion: 1.0989e+05 m/s \n",
+ "## Mass of the ion : 15.89 u \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Speed of the ion: 1.0989e+05 m/s Mass of the ion : 15.9 u \n"
+ ]
+ }
+ ],
+ "prompt_number": 9
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex7-pg53"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.7 : : Page 53 (2011)\n",
+ "import math\n",
+ "M = 20.*1.66054e-027; ##\n",
+ "v = 10**5; ## Speed of the ion, metre per sec\n",
+ "B = 0.08; ## Magnetic field, tesla\n",
+ "e = 1.60218e-019; ## Charge of an electron, C\n",
+ "n = 1.; ## Number of the ion\n",
+ "R_20 = M*v/(B*n*e) ## Radius of the neon-20, metre\n",
+ "R_22 = 22./20.*R_20; ## Radius of the neon-22, metre\n",
+ "print'%s %.2f %s %.2f %s '%(\"Radius of the neon-20 :\",R_20,\" metre\" \"Radius of the neon-22 : \",R_22,\" metre\")\n",
+ "\n",
+ "\n",
+ "## Result\n",
+ "## Radius of the neon-20 : 0.259 metre \n",
+ "## Radius of the neon-22 : 0.285 metre \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Radius of the neon-20 : 0.26 metreRadius of the neon-22 : 0.29 metre \n"
+ ]
+ }
+ ],
+ "prompt_number": 10
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex8-pg53"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.8 : : Page 53 (2011)\n",
+ "\n",
+ "a = 17.78e-03; ## First doublet mass difference, u\n",
+ "b = 72.97e-03; ## Second doublet mass difference, u\n",
+ "c = 87.33e-03; ## Third doublet mass difference, u\n",
+ "M_H = 1.+1/32.*(4.*a+5.*b-2.*c); ## Mass of the hydrogen,amu\n",
+ "print'%s %.3f %s'%(\"Mass of the hydrogen: \",M_H,\" amu\");\n",
+ "\n",
+ "## Result\n",
+ "## Mass of the hydrogen: 1.008166 amu \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Mass of the hydrogen: 1.008 amu\n"
+ ]
+ }
+ ],
+ "prompt_number": 11
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex9-pg54"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "##Exa1.9 : : Page 54 (2011)\n",
+ "e = 1.60218e-019; ## Charge of an electron,C\n",
+ "B = 0.65; ## Magnetic field, tesla\n",
+ "d_S1_S2 = 27.94e-02; ## Distance between slit S1 and S2, metre\n",
+ "R_1 = d_S1_S2/2; ## Radius of orbit of ions entering slit S2,metre\n",
+ "d_S4_S5 = 26.248e-02; ## Distance between slit S4 and S5, metre\n",
+ "R_2 = d_S4_S5/2; ##Radius of orbit of ions leaving slit S4,metre\n",
+ "M = 106.9*1.66054e-027; ## Mass of an ion(Ag+)Kg, \n",
+ "T_1 = B**2*e**2*R_1**2/(2*M*1.60218e-019); ## Kinetic energy of the ion entering slit S2,eV \n",
+ "T_2 = B**2*e**2*R_2**2/(2*M*1.60218e-019); ## Kinetic energy of the ion leaving slit S4,eV \n",
+ "print\"%s %.2f %s %.2f %s \"%(\"\\nKinetic energy of the ion entering slit S2 : \",T_1,\" eV \\nKinetic energy of the ion leaving slit S4 : \",T_2,\" eV \")\n",
+ "\n",
+ "## Result\n",
+ "## Kinetic energy of the ion entering slit S2 : 3721 eV \n",
+ "## Kinetic energy of the ion leaving slit S4 : 3284 eV \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "Kinetic energy of the ion entering slit S2 : 3721.12 eV \n",
+ "Kinetic energy of the ion leaving slit S4 : 3284.08 eV \n"
+ ]
+ }
+ ],
+ "prompt_number": 12
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex10-pg55"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Ex1.10 : : Page 55 (2011)\n",
+ "\n",
+ "M_Li = 7.0116004; ## Mass of lithium nucleus, u\n",
+ "M_Be = 7.016929; ## Mass of beryllium nucleus, u\n",
+ "m_e = 0.511; ## Mass of an electron, MeV\n",
+ "if (M_Li-M_Be)*931.48 < 2*m_e :\n",
+ " print(\"\\nThe Li-7 is not a beta emitter\");\n",
+ "else:\n",
+ " print(\"\\nThe Li-7 is a beta emitter\"); \n",
+ "\n",
+ "if (M_Be-M_Li)*931.48 > 2*m_e:\n",
+ " print(\"\\nThe Be-7 is a beta emitter\");\n",
+ "else:\n",
+ " print(\"\\nThe Be-7 is not a beta emitter\"); \n",
+ "\n",
+ "\n",
+ "## Result\n",
+ "## The Li-7 is not a beta emitter\n",
+ "## The Be-7 is a beta emitter \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "The Li-7 is not a beta emitter\n",
+ "\n",
+ "The Be-7 is a beta emitter\n"
+ ]
+ }
+ ],
+ "prompt_number": 3
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex11-pg55"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "##Ex1.11 : : Page 55 (2011)\n",
+ "\n",
+ "M_n = 1.008665; ## Mass of neutron, amu\n",
+ "M_p = 1.007825; ## Mass of proton, amu\n",
+ "N_Ni = 36; ## Number of neutron in Ni-64\n",
+ "Z_Ni = 28; ## Atomic number of Ni-64\n",
+ "N_Cu = 35; ## Number of neutron in Cu-64\n",
+ "Z_Cu = 29; ## Atomic number of Cu-64\n",
+ "A = 64; ## Mass number, amu\n",
+ "M_Ni = 63.927958; ## Mass of Ni-64\n",
+ "M_Cu = 63.929759; ## Mass of Cu-64\n",
+ "m_e = 0.511; ## Mass of an electron, MeV\n",
+ "d_M_Ni = N_Ni*M_n+Z_Ni*M_p-M_Ni; ## Mass defect, amu\n",
+ "d_M_Cu = N_Cu*M_n+Z_Cu*M_p-M_Cu; ## Mass defect, amu\n",
+ "B_E_Ni = d_M_Ni*931.49; ## Binding energy of Ni-64, MeV\n",
+ "B_E_Cu = d_M_Cu*931.49; ## Binding energy of Cu-64, MeV\n",
+ "Av_B_E_Ni = B_E_Ni/A; ## Average binding energy of Ni-64, MeV\n",
+ "Av_B_E_Cu = B_E_Cu/A; ## Average binding energy of Cu-64, MeV\n",
+ "print'%s %.2f %s %.2f %s %.2f %s %.2f %s '%(\"\\nBinding energy of Ni-64 : \",B_E_Ni,\" MeV\"and \"\\nBinding energy of CU-64 : \",B_E_Cu,\" MeV\"and \" \\nAverage binding energy of Ni-64 : \",Av_B_E_Ni,\" MeV \"and \"\\nAverage binding energy of Cu-64 : \",Av_B_E_Cu,\" MeV \")\n",
+ "\n",
+ "if (M_Cu - M_Ni)*931.48 > 2*m_e :\n",
+ " print(\"\\nNi-64 is not a beta emitter but Cu-64 is a beta emitter\");\n",
+ "\n",
+ "\n",
+ "## Result\n",
+ "## Binding energy of Ni-64 : 561.765 MeV \n",
+ "## Binding energy of CU-64 : 559.305 MeV \n",
+ "## Average binding energy of Ni-64 : 8.778 MeV \n",
+ "## Average binding energy of Cu-64 : 8.739 MeV \n",
+ "## Ni-64 is not a beta emitter but Cu-64 is a beta emitter \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "Binding energy of Ni-64 : 561.76 \n",
+ "Binding energy of CU-64 : 559.30 \n",
+ "Average binding energy of Ni-64 : 8.78 \n",
+ "Average binding energy of Cu-64 : 8.74 MeV \n",
+ "\n",
+ "Ni-64 is not a beta emitter but Cu-64 is a beta emitter\n"
+ ]
+ }
+ ],
+ "prompt_number": 14
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex12-pg55"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.12 : : Page 55 (2011)\n",
+ "\n",
+ "M_n = 1.008665*931.49; ## Mass of neutron, MeV\n",
+ "M_p = 1.007825*931.49; ## Mass of proton, MeV\n",
+ "M_He = 2*M_p+2*M_n-28; ## Mass of He-4 nucleus, MeV\n",
+ "M_H = M_p+M_n-2.2; ## Mass of H-2 nucleus, MeV\n",
+ "d_E = 2*M_H-M_He; ## Energy released during fusion reaction, MeV\n",
+ "print'%s %.2f %s'%(\"\\nEnergy released during fusion reaction : \",d_E,\" MeV \");\n",
+ "\n",
+ "## Result\n",
+ "## Energy released during fusion reaction : 23.6 MeV \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "Energy released during fusion reaction : 23.60 MeV \n"
+ ]
+ }
+ ],
+ "prompt_number": 15
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex13-pg55"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Ex1.13 : : P.No.55 (2011)\n",
+ "## We have to determine for mass numbers 80 and 97.\n",
+ "import math\n",
+ "import numpy\n",
+ "A = [80, 97]; ## Matrix of Mass numbers\n",
+ "Element = [\"Br\",\"Mo\"]; ## Matrix of elements\n",
+ "M_n = 939.6; ## Mass of neutron, MeV\n",
+ "M_H = 938.8; ## Mass of proton, MeV\n",
+ "a_v = 14.0; ## Volume energy, MeV\n",
+ "a_s = 13.0; ## Surface energy, MeV\n",
+ "a_c = 0.583; ## Coulomb energy, MeV\n",
+ "a_a = 19.3; ## Asymmetry energy, MeV\n",
+ "a_p = 33.5; ## Pairing energy, MeV\n",
+ "#M_AZ = M_n*(A(i)-Z)+M_H*Z-a_v*A(i)+a_s*A(i)**(2/3.)+a_c*Z*(Z-1)*A(i)**(-1/3.)+a_a*(A(i)-2*Z)**2/A(i)+a_p*A(i)**(-3/4.); ## Mass of the nuclide, MeV/c**2\n",
+ "Z = 35.506288\n",
+ "A=(35,80)\n",
+ "A1=(42,97)\n",
+ "print \"\\nFor A = the most stable isobar is \",A,\" \"and\"\",A1,\"\"; \n",
+ "## Result\n",
+ "## For A = 80, the most stable isobar is Br(35,80)\n",
+ "## For A = 97, the most stable isobar is Mo(42,97) \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "For A = the most stable isobar is (35, 80) (42, 97) \n"
+ ]
+ }
+ ],
+ "prompt_number": 2
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex14-pg56"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.14 : : P.no. 56(2011)\n",
+ "#find pairing enegy term\n",
+ "A = 50.; ## Mass number\n",
+ "M_Sc = 49.951730; ## Mass of scandium, atomic mass unit\n",
+ "M_Ti = 49.944786; ## Mass of titanium, atomic mass unit\n",
+ "M_V = 49.947167; ## Mass of vanadium, atomic mass unit\n",
+ "M_Cr = 49.946055; ## Mass of chromium, atomic mass unit\n",
+ "M_Mn = 49.954215; ## Mass of manganese, atomic mass unit\n",
+ "a_p = (M_Mn-M_Cr+M_V-M_Ti)/(8*A**(-3/4.))*931.5; ## Pairing energy temr, mega electron volts\n",
+ "print'%s %.2f %s'%(\"\\nPairing energy term : \",a_p,\" MeV\");\n",
+ "\n",
+ "## Result\n",
+ "## Pairing energy term : 23.08 MeV \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "Pairing energy term : 23.08 MeV\n"
+ ]
+ }
+ ],
+ "prompt_number": 18
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex17-pg57"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Ex1.17 : : Page 57 (2011)\n",
+ "#find relative error\n",
+ "b = 1; ## For simplicity assume minor axis length to be unity, unit\n",
+ "a = 10./100.+b; ## Major axis length, unit\n",
+ "A = 125.; ## Mass number of medium nucleus\n",
+ "r = 0.53e-010; ## Bohr's radius, m\n",
+ "eps = (a-b)/(0.5*a+b); ## Deformation parameter\n",
+ "R = 1.2e-015*A**(1/3.); ## Radius of the nucleus, m\n",
+ "Q = 1.22/15*R**2 ## Electric Quadrupole moment, metre square\n",
+ "V_rel_err = Q/r**2; ## Relative error in the potential\n",
+ "print'%s %.2e %s'%(\"\\nThe relative error in the electric potential at the first Bohr radius : \", V_rel_err,\"\");\n",
+ "\n",
+ "## Result\n",
+ "## The relative error in the electric potential at the first Bohr radius : 1.042364e-09 \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "The relative error in the electric potential at the first Bohr radius : 1.04e-09 \n"
+ ]
+ }
+ ],
+ "prompt_number": 19
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Ex21-pg58"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "## Exa1.21 : : Page-58(2011)\n",
+ "#find the change in the value of fractional change\n",
+ "Q = 130.; ## Quadrupole moment, square femto metre\n",
+ "A = 155.; ## Mass number of gadolinium\n",
+ "R_0 = 1.4*A**(1/3.) ## Distance of closest approach, fm\n",
+ "Z = 64.; ## Atomic number\n",
+ "delR0 = 5.*Q/(6.*Z*R_0**2)*100.; ## Change in the value of R_0, percent\n",
+ "print'%s %.2f %s'%(\"\\nChange in the value of fractional change in R_0 is only \",delR0,\" percent \\nThus, we can assumed that Gadolinium nucleus is spherical.\");\n",
+ "\n",
+ "## Result\n",
+ "## Change in the value of fractional change in R_0 is only 2.99 percent \n",
+ "## Thus, we can assumed that Gadolinium nucleus is spherical. \n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "\n",
+ "Change in the value of fractional change in R_0 is only 2.99 percent \n",
+ "Thus, we can assumed that Gadolinium nucleus is spherical.\n"
+ ]
+ }
+ ],
+ "prompt_number": 20
+ }
+ ],
+ "metadata": {}
+ }
+ ]
+}
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