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Part B Lab Go to PhET website. Click on Simulation Physics. Under Physics, choose Light & Radiation. Under Light & Radiation,
Part C Discovery Beyond what you have done with Bending Light/More Tools Simulation, make few new findings such changing medi
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Answer #1

Part B Lab
Following is a screen shot of 700 nm Measurement from the simulation

Ray Wave 700 nm - Material Air - Index of Refraction (n) 1.000 45.0° 45.0° Air Water Glass 0 0 30 60 T - 30 - Material Glass

Following is the completed data table from the given procedure in the lab manual

lambda1 theta2 n2m n2=n1*sin(theta1)/sin(theta2) c2' = c/n2
700 28.2 1.499 1.496361521 0.668288
500 28 1.499 1.506175959 0.663933
400 27.8 1.499 1.516138586 0.65957


Questions
1. lambda1 = 700 nm in air
lambda2 = lambda1/n2 = 700/1.5 = 466.66666666666 nm
speed in medium 2 is c/1.5 = 1.998666666*10^8 m/s
  
2.
now, v2 = v1 ( frequency does not change )
hence,
v2 = c/lambda1 = 4.2828571*10^14 Hz = v1
  
3. when lambda1 is changed, lambda2 changes, as well as theta 2 changes (because refractive index of a medium is actually dependent on the wavelength of the light being used)

Data table 2
The screen shot for theta = 41.8 deg measurement is as under

Ray O O Wave 650 nm Material Custom Index of Refraction (n) 1.500 41.8° 41.89 Air Water Glass 0 30 60 60 man 30 Material Cust

The completed data table according to the manual is as under

theta1 theta2 I1 I2 theta2c
30 48.5 10.55 89.45 48.59038
40 74.5 38.8 61.2 74.61857
41.8 87.2 83.81 16.19 88.85036
42 - 100 0

Questions
1. fvor theta1 > 41.8 deg, total internal reflection happens and the beam gets totally reflected and there is no refraction of light
2. by snells law
critical angle be a
then
sin(a)/sin(90) = 1/1.5
a = arcsin(0.66667)
a = 41.8103 deg

C. Discovery
On changing the refractive medium, the refractive index changes
increasing refractive index for constant wavelength increases the angle of refraction and the critical angle as well

On selecting the wave form of rays, we can see that the reflectred and the refracted beam are out of phases to each other when ligh is going from opitically rarer medium to optically denser medium
where as when it moves from optically denser medium to optically ratrer medium the refracted and the reflected rays are in phase

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