diff options
author | kinitrupti | 2017-05-12 18:40:35 +0530 |
---|---|---|
committer | kinitrupti | 2017-05-12 18:40:35 +0530 |
commit | d36fc3b8f88cc3108ffff6151e376b619b9abb01 (patch) | |
tree | 9806b0d68a708d2cfc4efc8ae3751423c56b7721 /Modern_Physics_By_G.Aruldas/Chapter19_1.ipynb | |
parent | 1b1bb67e9ea912be5c8591523c8b328766e3680f (diff) | |
download | Python-Textbook-Companions-d36fc3b8f88cc3108ffff6151e376b619b9abb01.tar.gz Python-Textbook-Companions-d36fc3b8f88cc3108ffff6151e376b619b9abb01.tar.bz2 Python-Textbook-Companions-d36fc3b8f88cc3108ffff6151e376b619b9abb01.zip |
Revised list of TBCs
Diffstat (limited to 'Modern_Physics_By_G.Aruldas/Chapter19_1.ipynb')
-rwxr-xr-x | Modern_Physics_By_G.Aruldas/Chapter19_1.ipynb | 291 |
1 files changed, 0 insertions, 291 deletions
diff --git a/Modern_Physics_By_G.Aruldas/Chapter19_1.ipynb b/Modern_Physics_By_G.Aruldas/Chapter19_1.ipynb deleted file mode 100755 index c8745970..00000000 --- a/Modern_Physics_By_G.Aruldas/Chapter19_1.ipynb +++ /dev/null @@ -1,291 +0,0 @@ -{
- "metadata": {
- "name": "",
- "signature": "sha256:9326f276d5dc99ce97d41c9ca0d5924dbd68f522091536657f41d8cfe038dc31"
- },
- "nbformat": 3,
- "nbformat_minor": 0,
- "worksheets": [
- {
- "cells": [
- {
- "cell_type": "heading",
- "level": 1,
- "metadata": {},
- "source": [
- "19: Nuclear reactions"
- ]
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example number 19.1, Page number 368"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#importing modules\n",
- "import math\n",
- "from __future__ import division\n",
- "\n",
- "#Variable declaration\n",
- "m2H=2.014102; #atomic mass of 2H(u)\n",
- "mn=1.008665; #mass of n(u)\n",
- "m63Cu=62.929599; #mass of 63Cu(u)\n",
- "m64Zn=63.929144; #mass of m64Zn(u)\n",
- "E=931.5; #energy(MeV)\n",
- "Kx=10; #energy of deutron(MeV)\n",
- "Ky=15; #energy of neutron(MeV)\n",
- "\n",
- "#Calculation\n",
- "Q=E*(m2H+m63Cu-mn-m64Zn); #Q-value(MeV)\n",
- "KY=Q+Kx-Ky; #kinetic energy(MeV)\n",
- "\n",
- "#Result\n",
- "print \"Q-value is\",round(Q,3),\"MeV\"\n",
- "print \"kinetic energy is\",round(KY,3),\"MeV\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "Q-value is 5.488 MeV\n",
- "kinetic energy is 0.488 MeV\n"
- ]
- }
- ],
- "prompt_number": 2
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example number 19.2, Page number 368"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#importing modules\n",
- "import math\n",
- "from __future__ import division\n",
- "\n",
- "#Variable declaration\n",
- "m19F=18.998404; #atomic mass of 19F(u)\n",
- "mH=1.007825; #mass of H(u)\n",
- "m19O=19.003577; #mass of 19O(u)\n",
- "mn=1.008665; #mass of n(u)\n",
- "E=931.5; #energy(MeV)\n",
- "\n",
- "#Calculation\n",
- "Q=E*(m19F+mn-mH-m19O); #Q-value(MeV)\n",
- "Kxmin=-Q*(1+(mn/m19F)); #threshold energy(MeV)\n",
- "\n",
- "#Result\n",
- "print \"Q-value is\",round(Q,4),\"MeV\"\n",
- "print \"threshold energy is\",round(Kxmin,2),\"MeV\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "Q-value is -4.0362 MeV\n",
- "threshold energy is 4.25 MeV\n"
- ]
- }
- ],
- "prompt_number": 5
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example number 19.3, Page number 373"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#importing modules\n",
- "import math\n",
- "from __future__ import division\n",
- "\n",
- "#Variable declaration\n",
- "mn=1.008665; #mass of n(u)\n",
- "mu=235.043924; #mass of 235U(u)\n",
- "mBa=140.91440; #mass of 141Ba(u)\n",
- "mKr=91.92630; #mass of Kr(u)\n",
- "E=931.5; #energy(MeV)\n",
- "\n",
- "#Calculation\n",
- "mr=mn+mu; #mass of reactants(u)\n",
- "mp=mBa+mKr+(3*mn); #mass of products(u)\n",
- "md=mr-mp; #mass difference(u)\n",
- "E=md*E; #energy released(MeV)\n",
- "\n",
- "#Result\n",
- "print \"energy released is\",round(E,1),\"MeV\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "energy released is 173.2 MeV\n"
- ]
- }
- ],
- "prompt_number": 19
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example number 19.4, Page number 373"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#importing modules\n",
- "import math\n",
- "from __future__ import division\n",
- "\n",
- "#Variable declaration\n",
- "E=200*10**6; #energy released(eV)\n",
- "e=1.6*10**-19; #conversion factor from J to eV\n",
- "P=300*10**6; #power(W)\n",
- "t=1; #time(s)\n",
- "\n",
- "#Calculation\n",
- "n=P*t/(E*e); #number of fissions per second\n",
- "\n",
- "#Result\n",
- "print \"number of fissions per second is\",n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "number of fissions per second is 9.375e+18\n"
- ]
- }
- ],
- "prompt_number": 20
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example number 19.5, Page number 378"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#importing modules\n",
- "import math\n",
- "from __future__ import division\n",
- "\n",
- "#Variable declaration\n",
- "m2H1=2*1.66*10**-27; #mass of proton(kg)\n",
- "E=931.5; #energy(MeV)\n",
- "m1=2.014102;\n",
- "m2=3.01609;\n",
- "mH=1.007825; #mass of H(u)\n",
- "\n",
- "#Calculation\n",
- "E=E*((2*m1)-m2-mH); #energy released(MeV)\n",
- "n=0.001/m2H1; #number of nuclei\n",
- "Eg=n*E/2; #energy released per gm(MeV)\n",
- "\n",
- "#Result\n",
- "print \"energy released per gm is\",round(Eg/10**23,2),\"*10**23 MeV\"\n",
- "print \"answer given in the book is wrong\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "energy released per gm is 6.02 *10**23 MeV\n",
- "answer given in the book is wrong\n"
- ]
- }
- ],
- "prompt_number": 31
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example number 19.6, Page number 379"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#importing modules\n",
- "import math\n",
- "from __future__ import division\n",
- "\n",
- "#Variable declaration\n",
- "k=8.99*10**9; #value of k(Nm**2/C**2)\n",
- "rd=1.5*10**-15; #radius of deuterium nucleus(m)\n",
- "rt=1.7*10**-15; #radius of tritium nucleus(m)\n",
- "e=1.6*10**-19; #conversion factor from J to eV\n",
- "KE=0.225; #kinetic energy for 1 particle(MeV)\n",
- "k=1.38*10**-23; #boltzmann constant(J/K)\n",
- "\n",
- "#Calculation\n",
- "K_E=k*e**2/(e*(rd+rt)); #kinetic energy of 2 particles(MeV)\n",
- "T=2*KE*e*10**6/(3*k); #temperature(K)\n",
- "\n",
- "#Result\n",
- "print \"temperature is\",round(T/10**9),\"*10**9 K\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "temperature is 2.0 *10**9 K\n"
- ]
- }
- ],
- "prompt_number": 35
- }
- ],
- "metadata": {}
- }
- ]
-}
\ No newline at end of file |