{ "metadata": { "celltoolbar": "Raw Cell Format", "name": "", "signature": "sha256:fad8e22fb99cc3e157ab8315172e2ff6ddae35bb6f49be764a49d2d1d3f70fcc" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Chapter 1: Interference" ] }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.1, Page number 1-16" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "i=45*math.pi/180 #angle of incidence\n", "u=1.33 #Refractive index of a soap film\n", "lamda=5.896*10**-7 #wavelength of required yellow light\n", "\n", "#Calculations:\n", "#u=sin i/sin r #Snell's law .So,\n", "r=math.asin(math.sin(i)/u) #angle of reflection\n", "\n", "#Now, condition for bright fringe is\n", "#2ut*cos r=(2n-1)lamda/2\n", "#Here n=1\n", "t=lamda/(2*2*u*math.cos(r)) #minimum thickness of film at which light will appear bright yellow\n", "print\"Minimum thickness of film at which light will appear bright yellow of required wavelength is =\",t,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Minimum thickness of film at which light will appear bright yellow of required wavelength is = 1.30853030399e-07 m\n" ] } ], "prompt_number": 1 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.2, Page number 1-16" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "theta=40./3600*math.pi/180 #angle of wedge in radians\n", "B=0.12*10**-2 #fringe spacing\n", "\n", "#Calculations:\n", "#We know, B=lam/(2*u*theta). Here u=1\n", "lamda=2*B*theta #wavelength of light used\n", "print\"Wavelength of light used is =\",lamda,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Wavelength of light used is = 4.65421133865e-07 m\n" ] } ], "prompt_number": 4 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.3, Page number 1-17" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "i=30*math.pi/180 #angle of incidence\n", "u=1.46 #Refractive index of a oil\n", "lamda=5.890*10**-7 #wavelength of required yellow light\n", "n=8 #eighth dark band\n", "\n", "#Calculations:\n", "#u=sin i/sin r #Snell's law .So,\n", "r=math.asin(math.sin(i)/u) #angle of reflection\n", "\n", "#Now, condition for dark fringe is\n", "#2ut*cos r=n*lamda\n", "t=n*lamda/(2*u*math.cos(r)) #thickness of film\n", "print\"Thickness of the film is =\",t,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of the film is = 1.71755887917e-06 m\n" ] } ], "prompt_number": 6 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.4, Page number 1-17" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "\n", "B=0.1*10**-2 #fringe spacing\n", "lamda=5.893*10**-7 #Wavelength of light\n", "u=1.52 #Refractive index of wedge\n", "\n", "#Calculations:\n", "#We know, B=lamda/(2*u*theta). Here u=1\n", "theta1=lamda/(2*u*B) #angle of wedge in radians\n", "theta=theta1*3600*180/math.pi #angle of wedge in seconds\n", "print\"Angle of wedge is =\",theta,\"seconds of an arc\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Angle of wedge is = 39.9841612899 seconds of an arc\n" ] } ], "prompt_number": 7 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.5, Page number 1-18" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "t=0.2/(100)**2*10**-2 #thickness of film in meter\n", "lamda=5.5*10**-7 #wavelength of light in meter\n", "r=0 #normal incidence\n", "n=1 #first band\n", "\n", "#Calculations:\n", "\n", "#Condition for dark fringe is\n", "#2ut*cos r =n*lamda\n", "u=n*lamda/(2*t*math.cos(r)) #Refractive index of a oil\n", "print\"Refractive index of a oil is =\",u\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Refractive index of a oil is = 1.375\n" ] } ], "prompt_number": 9 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.6, Page number 1-18" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "lamda=5.893*10**-7 #Wavelength of light\n", "u=1.42 #Refractive index of a soap film\n", "r=0 #normal incidence\n", "n=1 #first band\n", "\n", "#Calculations:\n", "\n", "#(i)\n", "#Condition for dark fringe is\n", "#2ut*cos r=n*lamda\n", "t1=n*lamda/(2*u*cos(r)) #thickness of film for dark black fringe\n", "print\"Thickness of the film for dark black fringe is =\",t1,\"m\"\n", "\n", "#(ii)\n", "#Now, condition for bright fringe is\n", "#2ut*cos r=(2n-1)lamda/2\n", "t2=lamda/(2*2*u*math.cos(r)) #Thickness of film for bright fringe\n", "print\"Thickness of film for bright fringe is =\",t2,\"m\"\n", "\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of the film for dark black fringe is = 2.075e-07 m\n", "Thickness of film for bright fringe is = 1.0375e-07 m\n" ] } ], "prompt_number": 4 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.7, Page number 1-19" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math \n", "#Given Data:\n", "i=30*math.pi/180 #angle of incidence\n", "u=1.43 #Refractive index of a soap film\n", "lamda=6*10**-7 #wavelength of light\n", "n=1 #For minimum thickness\n", "\n", "#Calculations:\n", "#u=sin i/sin r #Snell's law .So,\n", "r=(math.asin(math.sin(i)/u)) #angle of reflection\n", "\n", "#Now, condition of minima in transmitted system is\n", "#2ut*cos(r)=(2n-1)lamda/2\n", "t=lamda/(2*2*u*math.cos(r)) #minimum thickness of film\n", "print\"Minimum thickness of film is \",t,\"m\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Minimum thickness of film is 1.11962124395e-07 m\n" ] } ], "prompt_number": 49 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.8, Page number 1-19" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "\n", "lamda = 5893*10**-10 #Wavelength of light\n", "theta = 1 #assuming value of theta\n", "\n", "#We know, B=lamda/(2*u*theta). Here u=1\n", "B = lamda/(2*theta) #fringe spacing\n", "n=20 #interference fringes\n", "\n", "#Calculations:\n", "#t=n*B*tan(theta)\n", "t = 20*B*theta #Thickness of wire\n", "print\"Thickness of wire is =\",t,\"m\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of wire is = 5.893e-06 m\n" ] } ], "prompt_number": 2 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.9, Page number 1-20" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "u1=1.3 #Refractive index of oil\n", "u2=1.5 #Refractive index of glass\n", "lamda1=7*10**-7 #Wavelength of light\n", "lamda2=5*10**-7 #Wavelength of light\n", "\n", "#Calculations:\n", "\n", "#for finding value of n, solve:\n", "#(2n+1)*lamda1/2=(2(n+1)+1)*lamda2/2\n", "#We get,n=2\n", "n=2\n", "\n", "toil=(2*n+1)*lamda1/(2*u1*2) #thickness of oil layer\n", "print\"Thickness of oil layer is =\",toil,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of oil layer is = 6.73076923077e-07 m\n" ] } ], "prompt_number": 5 }, { "cell_type": "code", "collapsed": false, "input": [ "Example 1.10, Page number 1-21" ], "language": "python", "metadata": {}, "outputs": [] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "u1=1.2 #Refractive index of drop of oil\n", "u2=1.33 #Refractive index of water\n", "lamda=4.8*10**-7 #wavelength of light\n", "n=3 #order\n", "r=0 #normal incidence,so r=0\n", "\n", "#Calculations:\n", "t=n*lamda/(2*u1) #Thickness of oil drop\n", "print\"Thickness of oil drop is =\",t,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of oil drop is = 6e-07 m\n" ] } ], "prompt_number": 6 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.11, Page number 1-22" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "i=math.asin(4/5) #angle of incidence\n", "u=4/3 #Refractive index of a soap film\n", "lamda1=6.1*10**-7 #wavelength of light\n", "lamda2=6*10**-7 #wavelength of light\n", "\n", "#Calculations:\n", "#u=sin i/sin r #Snell's law .So,\n", "r=math.asin(math.sin(i)/u) #angle of reflection\n", "\n", "#Now, condition for dark band is\n", "#2ut*cos r=n*lamda\n", "#for consecutive bands, n=lamda2/(lamda1-lamda2). hence\n", "\n", "t=lamda2*lamda1/((lamda1-lamda2)*2*u*math.sqrt(1-(math.sin(i)/u)**2)) #thickness of film\n", "print\"Thickness of the film is =\",t,\"m\"\n", "\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of the film is = 1.83e-05 m\n" ] } ], "prompt_number": 55 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.12, Page number 1-40" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "n=10 #10th dark ring\n", "Dn=0.5*10**-2 #Diameter of ring\n", "lamda=6*10**-7 #wavelength of light\n", "\n", "#Calculations:\n", "#As Dn^2=4*n*R*lamda\n", "R=Dn**2/(4*n*lamda) #Radius of curvature of the lens\n", "print\"Radius of curvature of the lens is =\",R,\"m\"\n", "\n", "t=Dn**2/(8*R) #thickness of air film\n", "print\"Thickness of air film is =\",t,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Radius of curvature of the lens is = 1.04166666667 m\n", "Thickness of air film is = 3e-06 m\n" ] } ], "prompt_number": 9 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.13, Page number 1-41" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "\n", "B=0.25*10**-2 #fringe spacing\n", "lamda=5.5*10**-7 #Wavelength of light\n", "u=1.4 #Refractive index of wedge\n", "\n", "#Calculations:\n", "#We know, B=lamda/(2*u*theta).\n", "theta1=lamda/(2*u*B) #angle of wedge in radians\n", "theta=theta1*3600*180/math.pi #angle of wedge in seconds\n", "print\"Angle of wedge is =\",theta,\"seconds\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Angle of wedge is = 16.2065204908 seconds\n" ] } ], "prompt_number": 13 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.14, Page number 1-41" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "n=4 #4th dark ring\n", "m=12 #m=n+p\n", "D4=0.4*10**-2 #Diameter of 4th ring\n", "D12=0.7*10**-2 #Diameter of 12th ring\n", "\n", "#Calculations:\n", "\n", "#(Dn+p)^2-Dn^2=4*p*lamda*R\n", "#Solving, (D12^2-D4^2)/(D20^2-D4^2)\n", "#We get above value =1/2. Hence\n", "D20=math.sqrt(2*D12**2-D4**2) #Diameter of 20th ring\n", "print\"Diameter of 20th ring is =\",D20,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Diameter of 20th ring is = 0.00905538513814 m\n" ] } ], "prompt_number": 14 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.15, Page number 1-42" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "n=6 #6th bright ring\n", "D6=0.31*10**-2 #Diameter of 6th ring\n", "lamda=6*10**-7 #wavelength of light\n", "R=1 #Radius of curvature\n", "\n", "#Calculations:\n", "\n", "#Diameter of nth bright ring is \n", "#Dn^2=2(2n-1)*lamda*R/u. Hence\n", "u=2*(2*n-1)*lamda*R/(D6)**2 #Refractive index of liquid\n", "print\"Refractive index of liquid is =\",u\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Refractive index of liquid is = 1.37356919875\n" ] } ], "prompt_number": 15 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.16, Page number 1-42" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "lamda=6*10**-7 #wavelength of light\n", "k=0.125*10**-4 #k=D(n+1)^2-Dn^2.\n", "u=1 #Refractive index of medium between lens and plate\n", "#Calculations:\n", "\n", "#(i)\n", "lamda1=4.5*10**-7 #new wavelength of light\n", "#Difference between squres of diameters of successive rings is directly proportional to wavelength.So,\n", "k1=lamda1/lamda*k #new Difference between squres of diameters of successive rings after changing wavelength\n", "print\"New Difference between squres of diameters of successive rings after changing wavelength is =\",k1,\"m^2\"\n", "\n", "#(ii)\n", "u2=1.33 #Refractive index of liquid introduced between lens and plate\n", "#Difference between squres of diameters of successive rings is inversely proportional to Refractive index.so,\n", "k2=u/u2*k #new Difference between squres of diameters of successive rings after changing refractive index\n", "print\"New Difference between squres of diameters of successive rings after changing refrective index is =\",k2,\"m^2\"\n", "\n", "#(iii)\n", "#Difference between squres of diameters of successive rings is directly proportional to Radius of curvature.So,\n", "#after doubling radius of curvature,\n", "k3=2*k #new Difference between squres of diameters of successive rings after doubling radius of curvature\n", "print\"New Difference between squres of diameters of successive rings after doubling radius of curvature is =\",k3,\"m^2\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "New Difference between squres of diameters of successive rings after changing wavelength is = 9.375e-06 m^2\n", "New Difference between squres of diameters of successive rings after changing refrective index is = 9.3984962406e-06 m^2\n", "New Difference between squres of diameters of successive rings after doubling radius of curvature is = 2.5e-05 m^2\n" ] } ], "prompt_number": 16 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.17, Page number 1-43" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "Dn=0.225*10**-2 #Diameter of nth ring\n", "Dm=0.45*10**-2 #Diameter of (n+9)th ring\n", "lamda=6*10**-7 #wavelength of light\n", "R=0.9 #Radius of curvature\n", "p=9\n", "\n", "#Calculations:\n", "#(Dn+p)^2-Dn^2=4*p*lamda*R/u\n", "u=4*p*lamda*R/((Dm)**2-Dn**2) #Refractive index of liquid\n", "print\"Refractive index of liquid is =\",u\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Refractive index of liquid is = 1.28\n" ] } ], "prompt_number": 17 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.18, Page number 1-44" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "D10=0.5*10**-2 #Diameter of 10th ring\n", "lamda=5.5*10**-7 #wavelength of light\n", "u=1.25 #Refractive index of liquid\n", "\n", "\n", "#Calculations:\n", "#As Dn^2=4*n*R*lamda/u\n", "#Dn^2 is inversely proportional to refractive index.\n", "D10n=D10/math.sqrt(u) #new diameter of 10th ring after changing medium between lens and plate\n", "print\"new diameter of 10th ring after changing medium between lens and plate is =\",D10n,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "new diameter of 10th ring after changing medium between lens and plate is = 0.004472135955 m\n" ] } ], "prompt_number": 18 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.19, Page number 1-45" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "D5=0.336*10**-2 #Diameter of 5th ring\n", "D15=0.59*10**-2 #Diameter of 15th ring\n", "lamda=5.89*10**-7 #wavelength of light\n", "p=10 #n=5,n+p=15\n", "\n", "#Calculations:\n", "#(Dn+p)^2-Dn^2=4*p*lamdaR/u\n", "R=((D15)**2-D5**2)/(4*p*lamda) #Radius of curvature of the lens\n", "print\"Radius of curvature of the lens is =\",R,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Radius of curvature of the lens is = 0.998319185059 m\n" ] } ], "prompt_number": 20 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.20, Page number 1-45" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "n=10 #10th dark ring\n", "D10=0.6*10**-2 #Diameter of ring\n", "lamda=6*10**-7 #wavelength of light\n", "u=4./3 #Refractive index of water\n", "\n", "\n", "#Calculations:\n", "#As Dn^2=4*n*R*lamda/u\n", "R=(D10**2)*u/(4*n*lamda) #Radius of curvature of the lens\n", "print\"Radius of curvature of the lens is =\",R,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Radius of curvature of the lens is = 2.0 m\n" ] } ], "prompt_number": 27 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.20.1, Page number 1-52" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "i=45*math.pi/180 #angle of incidence\n", "u=1.2 #Refractive index of a film\n", "t=4*10**-7 #thickness of film\n", "\n", "#Calculations:\n", "#u=sin i/sin r #Snell's law .So,\n", "r=math.asin(math.sin(i)/u) #angle of reflection\n", "\n", "#Now, condition for dark fringe is\n", "#2ut*cos r=n*lamda\n", "lamda1=2*u*t*math.cos(r)/1 #n=1\n", "print\"For n=1 wavelength is =\",lamda1,\"m\"\n", "print\"This is in the visible spectrum and it will remain absent.\" \n", "\n", "lamda2=2*u*t*math.cos(r)/2 #n=2\n", "print\"For n=2 wavelength is =\",lamda2,\"m\"\n", "print\"This is not in the visible spectrum\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "For n=1 wavelength is = 7.75628777187e-07 m\n", "This is in the visible spectrum and it will remain absent.\n", "For n=2 wavelength is = 3.87814388593e-07 m\n", "This is not in the visible spectrum\n" ] } ], "prompt_number": 30 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.20.2, Page number 1-53" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "r=45*math.pi/180 #angle of refraction\n", "u=1.45 #Refractive index of a medium\n", "lamda=5.5*10**-7 #wavelength of required yellow light\n", "n=1\n", "\n", "#Calculations:\n", "\n", "#Now, condition for dark fringe is\n", "#2ut*cos r=n*lamda\n", "t=n*lamda/(2*u*math.cos(r)) #thickness of thin medium\n", "print\"Thickness of the thin medium is =\",t,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of the thin medium is = 2.68212917002e-07 m\n" ] } ], "prompt_number": 31 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.21, Page number 1-45" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "u=1.33 #Refractive index of a soap film\n", "r=0 #normal incidence\n", "t=5*10**-7 #thickness of film\n", "\n", "#Calculations:\n", "\n", "#Now, condition for maxima is\n", "#2ut*cos r=(2n-1)lamda/2\n", "lamda1=4*u*t*math.cos(r)/(2*1-1) #n=1\n", "print\"For n=1 wavelength is =\",lamda1,\"m\"\n", "lamda2=4*u*t*math.cos(r)/(2*2-1) #n=2\n", "print\"For n=2 wavelength is =\",lamda2,\"m\"\n", "lamda3=4*u*t*math.cos(r)/(2*3-1) #n=3\n", "print\"For n=3 wavelength is =\",lamda3,\"m\"\n", "lamda4=4*u*t*math.cos(r)/(2*4-1) #n=4\n", "print\"For n=4 wavelength is =\",lamda4,\"m\"\n", "\n", "print\"Out of these wavelengths wavelength for n=3 lies in the visible spectrum.\"\n", "print\"Hence, wavelength for n=3 is the most reflected wavelength.\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "For n=1 wavelength is = 2.66e-06 m\n", "For n=2 wavelength is = 8.86666666667e-07 m\n", "For n=3 wavelength is = 5.32e-07 m\n", "For n=4 wavelength is = 3.8e-07 m\n", "Out of these wavelengths wavelength for n=3 lies in the visible spectrum.\n", "Hence, wavelength for n=3 is the most reflected wavelength.\n" ] } ], "prompt_number": 32 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.22, Page number 1-46" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "u=1.5 #Refractive index of a oil\n", "lamda=5.88*10**-7 #wavelength of required yellow light\n", "n=1 #for smallest thickness\n", "r=60*math.pi/180 #angle of reflection\n", "\n", "#Calculations:\n", "\n", "#Now, condition for dark fringe is\n", "#2ut*cos r=n*lamda\n", "t=n*lamda/(2*u*math.cos(r)) #thickness of film\n", "print\"Thickness of the film is =\",t,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Thickness of the film is = 3.92e-07 m\n" ] } ], "prompt_number": 33 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.23, Page number 1-46" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "theta=20./3600*math.pi/180 #angle of wedge in radians\n", "B=0.25*10**-2 #fringe spacing\n", "u=1.4 #Refractive index of film\n", "\n", "#Calculations:\n", "#We know, B=lamda/(2*u*theta).\n", "lamda=2*B*theta*u #wavelength of light\n", "print\"Wavelength of light is =\",lamda,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Wavelength of light is = 6.78739153553e-07 m\n" ] } ], "prompt_number": 35 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.24, Page number 1-47" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "#Dn=2*D40\n", "\n", "#Calculations:\n", "#As Dn^2 = 4*n*R*lamda/u and Dn^2 = 4*D40^2\n", "#i.e. 4*n*R*lamda/u = 4*4*40*R*lamda/u .hence,\n", "n=4*40 #order of the required ring\n", "print\"Order of the dark ring which will have double the diameter of that of 40th ring is =\",n\n", " \n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Order of the dark ring which will have double the diameter of that of 40th ring is = 160\n" ] } ], "prompt_number": 36 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.25, Page number 1-47" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "lamda1=6*10**-7 #wavelength of light\n", "lamda2=4.5*10**-7 #wavelength of light\n", "R=0.9 #Radius of curvature\n", "\n", "#Calculations:\n", "#As Dn^2=4*n*R*lamda.\n", "#Dn^2=D(n+1)^2 for different wavelengths.we get,\n", "n=lamda2/(lamda1-lamda2) #nth dark ring due to lam1 which coincides with (n+1)th dark ring due lamda2\n", "D3=math.sqrt(4*n*R*lamda1) #diameter of 3rd dark ring for lamda1\n", "print\"Diameter of 3rd dark ring for lam1 is =\",D3,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Diameter of 3rd dark ring for lam1 is = 0.00254558441227 m\n" ] } ], "prompt_number": 38 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.26, Page number 1-48" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "i=45*math.pi/180 #angle of incidence\n", "u=4./3 #Refractive index of soap film\n", "lamda=5*10**-7 #wavelength of light\n", "t=1.5*10**-6 #thickness of film\n", "\n", "#Calculations:\n", "#u=sin i/sin r #Snell's law .So,\n", "r=math.asin(math.sin(i)/u) #angle of reflection\n", "\n", "#Now, condition for dark band is\n", "#2ut*cos r=n*lamda\n", "n=2*u*t*math.cos(r)/lamda #order of band\n", "print\"order of dark band is =\",n\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "order of dark band is = 6.78232998313\n" ] } ], "prompt_number": 39 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.27, Page number 1-49" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "D5=0.336*10**-2 #Diameter of 5th ring\n", "D15=0.59*10**-2 #Diameter of 15th ring\n", "lamda=5.89*10**-7 #wavelength of light\n", "p=10 #n=5,n+p=15\n", "\n", "#Calculations:\n", "#(Dn+p)^2-Dn^2=4*p*lamda*R/u\n", "R=((D15)**2-D5**2)/(4*p*lamda) #Radius of curvature of the lens\n", "print\"Radius of curvature of the lens is =\",R,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Radius of curvature of the lens is = 0.998319185059 m\n" ] } ], "prompt_number": 40 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.29, Page number 1-50" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#As Dn^2=4*n*R*lamda.\n", "#thus, Dn is directly proportional to sqaure root of n\n", "D5=math.sqrt(5) #D5 is directly proportional to sqaure root of 5\n", "D4=math.sqrt(4) #D4 is directly proportional to sqaure root of 4\n", "k1=D5-D4\n", "print\"Separation between D5 and D4 is directly proportional to =\",k1\n", "\n", "D80=math.sqrt(80) #D80 is directly proportional to sqaure root of 80\n", "D79=math.sqrt(79) #D79 is directly proportional to sqaure root of 79\n", "k2=D80-D79\n", "print\"Separation between D80 and D79 is directly proportional to =\",k2\n", "\n", "print\"Thus, (D80-D79) < (D5-D4). Hence proved.\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Separation between D5 and D4 is directly proportional to = 0.2360679775\n", "Separation between D80 and D79 is directly proportional to = 0.0560774926836\n", "Thus, (D80-D79) < (D5-D4). Hence proved.\n" ] } ], "prompt_number": 41 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.30, Page number 1-51" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#Given Data:\n", "D5=0.336*10**-2 #Diameter of 5th ring\n", "D15=0.59*10**-2 #Diameter of 15th ring\n", "p=10 #n=5,n+p=15\n", "R=1 #Radius of curvature\n", "\n", "#Calculations:\n", "#(Dn+p)^2-Dn^2=4*p*lamda*R/u\n", "lamda=((D15)**2-D5**2)/(4*p*R) #Wavelength of light\n", "print\"Wavelength of light is =\",lamda,\"m\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Wavelength of light is = 5.8801e-07 m\n" ] } ], "prompt_number": 42 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 1.31, Page number 1-51" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "\n", "#Condition for bright band is\n", "#2ut*cos r = (2n-1)*lamda1\n", "\n", "#for consecutive bands, 2n=(lamda1+lamda2)/(lamda1-lamda).\n", "#thus, 2ut*cos r = lamda2*lamda1/(lamda1-lamda2)\n", "\n", "#And, thicknessof film \n", "#t= lamda2*lamda1/((2*u*cosr)(lamda1-lamda2))\n", "print\"Hence expression for thickness of film is obtained.\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Hence expression for thickness of film is obtained.\n" ] } ], "prompt_number": 56 }, { "cell_type": "code", "collapsed": false, "input": [], "language": "python", "metadata": {}, "outputs": [] } ], "metadata": {} } ] }