summaryrefslogtreecommitdiff
path: root/1397/CH1
diff options
context:
space:
mode:
authorpriyanka2015-06-24 15:03:17 +0530
committerpriyanka2015-06-24 15:03:17 +0530
commitb1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (patch)
treeab291cffc65280e58ac82470ba63fbcca7805165 /1397/CH1
downloadScilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.gz
Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.bz2
Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.zip
initial commit / add all books
Diffstat (limited to '1397/CH1')
-rwxr-xr-x1397/CH1/EX1.1/1_1.sce13
-rwxr-xr-x1397/CH1/EX1.10/1_10.sce8
-rwxr-xr-x1397/CH1/EX1.11/1_11.sce8
-rwxr-xr-x1397/CH1/EX1.12/1_12.sce9
-rwxr-xr-x1397/CH1/EX1.13/1_13.sce9
-rwxr-xr-x1397/CH1/EX1.14/1_14.sce7
-rwxr-xr-x1397/CH1/EX1.15/1_15.sce9
-rwxr-xr-x1397/CH1/EX1.16/1_16.sce10
-rwxr-xr-x1397/CH1/EX1.17/1_17.sce7
-rwxr-xr-x1397/CH1/EX1.18/1_18.sce14
-rwxr-xr-x1397/CH1/EX1.19/1_19.sce10
-rwxr-xr-x1397/CH1/EX1.2/1_2.sce8
-rwxr-xr-x1397/CH1/EX1.20/1_20.sce8
-rwxr-xr-x1397/CH1/EX1.21/1_21.sce8
-rwxr-xr-x1397/CH1/EX1.22/1_22.sce7
-rwxr-xr-x1397/CH1/EX1.23/1_23.sce9
-rwxr-xr-x1397/CH1/EX1.24/1_24.sce8
-rwxr-xr-x1397/CH1/EX1.25/1_25.sce9
-rwxr-xr-x1397/CH1/EX1.26/1_26.sce8
-rwxr-xr-x1397/CH1/EX1.27/1_27.sce8
-rwxr-xr-x1397/CH1/EX1.28/1_28.sce9
-rwxr-xr-x1397/CH1/EX1.3/1_3.sce10
-rwxr-xr-x1397/CH1/EX1.4/1_4.sce9
-rwxr-xr-x1397/CH1/EX1.5/1_5.sce8
-rwxr-xr-x1397/CH1/EX1.6/1_6.sce8
-rwxr-xr-x1397/CH1/EX1.7/1_7.sce8
-rwxr-xr-x1397/CH1/EX1.8/1_8.sce8
-rwxr-xr-x1397/CH1/EX1.9/1_9.sce8
28 files changed, 245 insertions, 0 deletions
diff --git a/1397/CH1/EX1.1/1_1.sce b/1397/CH1/EX1.1/1_1.sce
new file mode 100755
index 000000000..a59904c38
--- /dev/null
+++ b/1397/CH1/EX1.1/1_1.sce
@@ -0,0 +1,13 @@
+//clc();
+clear;
+// To calculate the intensity ratio of bright and dark fringes
+I1=1;
+I2=25;
+// Intensity is directly proportional to square of the amplitude
+A1=sqrt(I1);
+A2=sqrt(I2);
+Imax=(A1+A2)^2;
+Imin=(A1-A2)^2;
+I=Imax/Imin;
+printf("The intensity ratio of bright and dark fringes is %f",I);
+
diff --git a/1397/CH1/EX1.10/1_10.sce b/1397/CH1/EX1.10/1_10.sce
new file mode 100755
index 000000000..ef32a7f6f
--- /dev/null
+++ b/1397/CH1/EX1.10/1_10.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To determine the refractive index of the transparent sheet in Newton's ring experiment
+lambda=5460*10^(-8); //wavelength of light in centimetres
+t=6.3*10^(-4); //thickness of the transparent material in centimetres
+n=6;
+mew=((n*lambda)/t)+1;
+printf("the refractive index of the transparent sheet when the central bright fringe is occupied by the 6th bright fringe is mew=%f",mew);
diff --git a/1397/CH1/EX1.11/1_11.sce b/1397/CH1/EX1.11/1_11.sce
new file mode 100755
index 000000000..59f7b93cd
--- /dev/null
+++ b/1397/CH1/EX1.11/1_11.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To determine the thickness of the glass plate
+mew=1.56; //refractive index of the glass plate
+lambda=5000*10^(-8); //wavelength of the light in centimetres
+n=16;
+t=(n*lambda)/(mew-1);
+printf("thickness of the glass plate in centimetres when 16 fringes are displaced is %f cm",t);
diff --git a/1397/CH1/EX1.12/1_12.sce b/1397/CH1/EX1.12/1_12.sce
new file mode 100755
index 000000000..ae0302829
--- /dev/null
+++ b/1397/CH1/EX1.12/1_12.sce
@@ -0,0 +1,9 @@
+//clc();
+clear;
+// To determine the thickness of the glass plate
+lambda=6000*10^(-8); //wavelength of parallel beam of light in centimetres
+mew=1.5; //refractive index of glass plate
+r=50; //angle of refraction in degrees
+n=1; //for least thickness
+t=(n*lambda)/(2*mew*cosd(r));
+printf("the least thickness of the glass plate in centimetres which will appear dark by reflection is %f cm",t);
diff --git a/1397/CH1/EX1.13/1_13.sce b/1397/CH1/EX1.13/1_13.sce
new file mode 100755
index 000000000..71040982c
--- /dev/null
+++ b/1397/CH1/EX1.13/1_13.sce
@@ -0,0 +1,9 @@
+//clc();
+clear;
+// To calculate the thickness of the glass plate
+lambda=5000*10^(-8); //wavelength of light in centimetres
+n=6; //shift of the central range or the ratio between S and beeta
+mew=1.5; //refractive index of glass plate
+t=(n*lambda)/(mew-1);
+printf("the thickness of the glass plate when the central fringe is shifted to the position of 6th bright fringe is %f cm",t);
+
diff --git a/1397/CH1/EX1.14/1_14.sce b/1397/CH1/EX1.14/1_14.sce
new file mode 100755
index 000000000..df76bc18b
--- /dev/null
+++ b/1397/CH1/EX1.14/1_14.sce
@@ -0,0 +1,7 @@
+//clc();
+clear;
+// To determine the refractive index of liquid in Newton's ring
+D8=1.42; //diameter of the 8th ring in centimetres
+D8new=1.25; //new diameter of the 8th ring in centimetres
+mew=(D8^2)/(D8new^2);
+printf("refractive index of the liquid when the liquid is intoduced between the lens and glass plate is %f",mew);
diff --git a/1397/CH1/EX1.15/1_15.sce b/1397/CH1/EX1.15/1_15.sce
new file mode 100755
index 000000000..87153f5d9
--- /dev/null
+++ b/1397/CH1/EX1.15/1_15.sce
@@ -0,0 +1,9 @@
+//clc();
+clear;
+// To determine the thickness of the thinnest film
+n=1;
+lambda=6000*10^(-8); //wavelength of yellow light in centimetres
+mew=1.33; //refractive index of the film
+r=0; //angle of refraction in degrees
+t=(n*lambda)/(2*mew*cosd(r)*10^(-2));
+printf("thickness of the thinnest film in which destructive interference takes place is %f cm",t);
diff --git a/1397/CH1/EX1.16/1_16.sce b/1397/CH1/EX1.16/1_16.sce
new file mode 100755
index 000000000..82bdedca8
--- /dev/null
+++ b/1397/CH1/EX1.16/1_16.sce
@@ -0,0 +1,10 @@
+//clc();
+clear;
+// To determine the radius of curvature of plano convex lens
+lambda=6000*10^(-8); //wavelength of light in centimetres
+m=18;
+n=8;
+Dm=0.65; //diameter of 18th ring in centimetres
+Dn=0.35; //diameter of 8th ring in centimetres
+R=(Dm^2-Dn^2)/(4*lambda*(m-n));
+printf("Radius of curvature of the plano convex lens when the wavelength of light used is 6000 Armstrong is %f cm",R)
diff --git a/1397/CH1/EX1.17/1_17.sce b/1397/CH1/EX1.17/1_17.sce
new file mode 100755
index 000000000..ce22f2ad9
--- /dev/null
+++ b/1397/CH1/EX1.17/1_17.sce
@@ -0,0 +1,7 @@
+//clc();
+clear;
+// To determine the refractive index of the liquid
+D12air=1.45; //diameter of 12th ring in air medium
+D12liq=1.25; //diameter of 12th ring in liquid
+mew=(D12air^2)/(D12liq^2);
+printf("refractive index of the liquid when liquid is introduced between the lens and glass plate is %f",mew);
diff --git a/1397/CH1/EX1.18/1_18.sce b/1397/CH1/EX1.18/1_18.sce
new file mode 100755
index 000000000..cc66e2cf0
--- /dev/null
+++ b/1397/CH1/EX1.18/1_18.sce
@@ -0,0 +1,14 @@
+//clc();
+clear;
+//To determine the diameter of a ring in Newton's rings experiment
+D5=0.3; //diameter of 5th ring in centimetres
+D15=0.62; //diameter of 15th ring in centimetres
+//The principle used here is Dm^2-Dn^2=4*lambda*R*(m-n).
+//the product lambda*R is constant hence it can be eliminated.
+aLHS=D15^2-D5^2;
+aRHS=4*(15-5); //By substituting the values of m and n in the principle equation
+bRHS=4*(25-5); //By substituting the values of m and n in the principle equation
+c=bRHS/aRHS;
+D25=sqrt((c*aLHS)+D5^2);
+printf("diameter of 25th ring is %f cm",D25);
+
diff --git a/1397/CH1/EX1.19/1_19.sce b/1397/CH1/EX1.19/1_19.sce
new file mode 100755
index 000000000..78bb66c3e
--- /dev/null
+++ b/1397/CH1/EX1.19/1_19.sce
@@ -0,0 +1,10 @@
+//clc();
+clear;
+//To determine the radius of curvature of convex lens
+lambda=5890*10^(-8); //wavelength in centimetres
+m=15;
+n=5;
+Dm=0.590; //diameter of 15th ring in centimetres
+Dn=0.336; //diameter of 5th ring in centimetres
+R=(Dm-Dn)/(4*lambda*(m-n));
+printf("radius of curvature of convex lens is %f cm",R);
diff --git a/1397/CH1/EX1.2/1_2.sce b/1397/CH1/EX1.2/1_2.sce
new file mode 100755
index 000000000..1b042fbf4
--- /dev/null
+++ b/1397/CH1/EX1.2/1_2.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To determine the order that will be visible at a point
+n1=21;
+lambda1=6000*10^(-8); // The 21st order maximum is observed for source of light in centimetres
+lambda2=4500*10^(-8);
+n2=(n1*lambda1)/(lambda2);
+printf("The order that will be visible if the source is replaced by 4500 Armstrong is %f",n2);
diff --git a/1397/CH1/EX1.20/1_20.sce b/1397/CH1/EX1.20/1_20.sce
new file mode 100755
index 000000000..2c6a840a4
--- /dev/null
+++ b/1397/CH1/EX1.20/1_20.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+//To determine the wavelength of the light used
+R=70; //radius of curvature of the lens in centimetres
+n=10;
+Dn=0.433 //diameter of 10th dark ring in centimetres
+lambda=(Dn^2)/(4*R*n);
+printf("the wavelength of the light used when a convex lens is exposed by a monochromatic light is %f cm",lambda);
diff --git a/1397/CH1/EX1.21/1_21.sce b/1397/CH1/EX1.21/1_21.sce
new file mode 100755
index 000000000..941e73c35
--- /dev/null
+++ b/1397/CH1/EX1.21/1_21.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+//To determine the slit width
+theta=15; //angle in degrees
+lambda=6500*10^(-8); //wavelength in centimetres
+n=1;
+a=(n*lambda)/sind(theta);
+printf("slit width illuminated by white light is %f cm",a);
diff --git a/1397/CH1/EX1.22/1_22.sce b/1397/CH1/EX1.22/1_22.sce
new file mode 100755
index 000000000..e16d4ae3e
--- /dev/null
+++ b/1397/CH1/EX1.22/1_22.sce
@@ -0,0 +1,7 @@
+//clc();
+clear;
+//To determine the wavelength of light
+theta=15; //first diffraction maxima in degrees
+a=2.5*10^(-6); //slit width in metres
+lambda=(a*sind(theta)*10^10)/1.43;
+printf("wavelength of light is %f Armstrong",lambda);
diff --git a/1397/CH1/EX1.23/1_23.sce b/1397/CH1/EX1.23/1_23.sce
new file mode 100755
index 000000000..c8eb866e6
--- /dev/null
+++ b/1397/CH1/EX1.23/1_23.sce
@@ -0,0 +1,9 @@
+//clc();
+clear;
+//To determine the wavelength of spectral line
+n=2;
+N=4250; //grating in lines per centimetre
+theta=30; //angle in degrees
+e=1/N;
+lambda=(e*sind(theta)*10^8)/n;
+printf("wavelength of the spectral line when a plane transmission grating is illuminated with a sodium light is %f Armstrong",lambda);
diff --git a/1397/CH1/EX1.24/1_24.sce b/1397/CH1/EX1.24/1_24.sce
new file mode 100755
index 000000000..6c1bf33cd
--- /dev/null
+++ b/1397/CH1/EX1.24/1_24.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+//To determine the angular seperation
+lambda=600*10^(-9); //wavelength of light in metres
+a=1*10^(-6); //slit width in metres
+n=1;
+theta=asind((n*lambda)/a);
+printf("the angular seperation between the first order minima and central maxima of either side is %f degrees",theta);
diff --git a/1397/CH1/EX1.25/1_25.sce b/1397/CH1/EX1.25/1_25.sce
new file mode 100755
index 000000000..283b569c1
--- /dev/null
+++ b/1397/CH1/EX1.25/1_25.sce
@@ -0,0 +1,9 @@
+//clc();
+clear;
+//To determine the visible number of orders
+N=10520; //grating lines in lines per centimetre
+theta=90; //angle in degrees
+lambda=5*10^(-5); //wavelength of light in centimetres
+e=1/N;
+n=(e*sind(theta))/lambda;
+printf("the number of orders visible in grating spectra is %f",n);
diff --git a/1397/CH1/EX1.26/1_26.sce b/1397/CH1/EX1.26/1_26.sce
new file mode 100755
index 000000000..34a803dc6
--- /dev/null
+++ b/1397/CH1/EX1.26/1_26.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+//To determine the slit width
+x=4.2*10^(-3); //distance between central max to first max in metres
+D=0.6; //distance between screen and slit in metres
+lambda=6000*10^(-10); //wavelength of light in metres
+d=(D*lambda)/x;
+printf("the slit width in a single slit diffraction pattern is %f m",d);
diff --git a/1397/CH1/EX1.27/1_27.sce b/1397/CH1/EX1.27/1_27.sce
new file mode 100755
index 000000000..f3ea1e30c
--- /dev/null
+++ b/1397/CH1/EX1.27/1_27.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+//To calculate the possible order of spectra
+N=5.905*10^3; //grating lines in lines per centimetre
+lambda=6000*10^(-8); //wavelength of light in centimetres
+d=1/N;
+m=d/lambda;
+printf("the possible order of spectra with a plane transmission grating is %f",m);
diff --git a/1397/CH1/EX1.28/1_28.sce b/1397/CH1/EX1.28/1_28.sce
new file mode 100755
index 000000000..1e40e1087
--- /dev/null
+++ b/1397/CH1/EX1.28/1_28.sce
@@ -0,0 +1,9 @@
+//clc();
+clear;
+//To determine the wavelength of light in Fraulhofer double slit diffraction
+D=150; //distance between slit and screen in centimetres
+d=0.03; //seperation between slits in centimetres
+beeta=0.3; //fringe seperation in centimetres
+lambda=(beeta*d*10^8)/D;
+printf("wavelength of light if fringe seperation is 0.3 cm is %f Armstrong",lambda);
+
diff --git a/1397/CH1/EX1.3/1_3.sce b/1397/CH1/EX1.3/1_3.sce
new file mode 100755
index 000000000..227d46298
--- /dev/null
+++ b/1397/CH1/EX1.3/1_3.sce
@@ -0,0 +1,10 @@
+//clc();
+clear;
+// To determine the slit seperation in Young's double slit experiment
+lambda=5100*10^(-8); //A source of light in centimetres
+D=200; // Seperation between screen and slit in centimetres
+beeta=0.01; // Overall seperation from double slit in metres
+d=(lambda*D)/beeta;
+printf("The seperation between slits if the source of light is incident from a narrow slit on a double slit is %f m",d);
+
+
diff --git a/1397/CH1/EX1.4/1_4.sce b/1397/CH1/EX1.4/1_4.sce
new file mode 100755
index 000000000..8f19da8a8
--- /dev/null
+++ b/1397/CH1/EX1.4/1_4.sce
@@ -0,0 +1,9 @@
+//clc();
+clear;
+// To determine the thickness of the mica sheet
+mew=1.58; // Refractive index of mica sheet
+d=0.1; // Seperation between slits in centimetres
+x=0.2; // Fringe shifted by a distance in centimetres
+D=50; // Distance of the screen from slits in centimetres
+t=(x*d)/(D*(mew-1));
+printf("The thickness of the mica sheet is %f cm",t);
diff --git a/1397/CH1/EX1.5/1_5.sce b/1397/CH1/EX1.5/1_5.sce
new file mode 100755
index 000000000..7a8f29338
--- /dev/null
+++ b/1397/CH1/EX1.5/1_5.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To determine the fringe width
+lambda=5000*10^(-8); //Wavelength of light in centimetres
+D=50; // Distance between the slit and screen in centimetres
+d=0.05; // Seperation between two slits in centimetres
+beeta=(lambda*D)/d;
+printf("the fringe width is %f cm",beeta);
diff --git a/1397/CH1/EX1.6/1_6.sce b/1397/CH1/EX1.6/1_6.sce
new file mode 100755
index 000000000..1703f30cd
--- /dev/null
+++ b/1397/CH1/EX1.6/1_6.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To determine the wavelength of source of light
+beeta=0.30; // fringe spacing in centimtres
+d=0.04; // distance between two slits in centimtres
+D=180; // distance between the slit and screen in centimetres
+lambda=(beeta*d*10^8)/D;
+printf("the wavelength of source of light is %f Armstrong",lambda);
diff --git a/1397/CH1/EX1.7/1_7.sce b/1397/CH1/EX1.7/1_7.sce
new file mode 100755
index 000000000..264bb84a1
--- /dev/null
+++ b/1397/CH1/EX1.7/1_7.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To calculate the wavelength of monochromatic light
+beeta=0.04; // fringe width in centimetres
+d=0.1; // seperation between slits in centimetres
+D=80; //distance between slits and screen in centimetres
+lambda=(d*beeta*10^8)/D;
+printf("the wavelength of monochromatic light is %f Armstrong",lambda);
diff --git a/1397/CH1/EX1.8/1_8.sce b/1397/CH1/EX1.8/1_8.sce
new file mode 100755
index 000000000..1afd3bf89
--- /dev/null
+++ b/1397/CH1/EX1.8/1_8.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To determine the fringe width
+lambda=5000*10^(-8); //wavelength of monochromatic light in centimetres
+d=0.05; // seperation between two slits in centimetres
+D=50; // distance between slit and screen in centimetres
+beeta=(lambda*D)/d;
+printf("the fringe width is %f cm",beeta);
diff --git a/1397/CH1/EX1.9/1_9.sce b/1397/CH1/EX1.9/1_9.sce
new file mode 100755
index 000000000..92a50977d
--- /dev/null
+++ b/1397/CH1/EX1.9/1_9.sce
@@ -0,0 +1,8 @@
+//clc();
+clear;
+// To determine the thickness of a soap film
+mew=1.33; //refractive index of soap film
+n=2;
+lambda=7000*10^(-8); //wavelength of red light in centimetres
+t=(((2*n)+1)*(lambda/2))/(2*mew);
+printf("thickness of the soap film which gives constructive second order interference is %f cm",t);