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Irina-Kira [14]
3 years ago
6

Light enters a transparent material from air at 30.0° to the normal. It continues within the material at the angle of refraction

of 23.0°. What is the critical angle for total internal reflection when this material is surrounded by air?
Physics
1 answer:
nikdorinn [45]3 years ago
8 0

Answer:

The value is c = 51.38 ^o

Explanation:

From the question we are told that

    The angle of incidence is  \theta_i = 30^o

    The angle of refraction is  \theta_r  =  23^o

     

Generally at the point where the light enters the material ,  from Snell's law  we have that

          n  =  \frac{sin (\theta_i)}{sin (\theta_{r})}

Here  n is the refractive index of the material

=>       n  =  \frac{sin (30)}{sin (23)}  

=>       n  =  1.28  

Generally for total internal  reflection , the critical angel is evaluated using Snell law as follows

          n  =  \frac{sin (90)}{sin (c)}

=>       1.28 *  sin (c)  =  sin(90)  

=>      c =  sin^{-1} [0.7813 ]

=>    c = 51.38 ^o

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(a) How many fringes appear between the first diffraction-envelope minima to either side of the central maximum in a double-slit
Ainat [17]

Answer:

a

The number of fringe is  z  = 3 fringes

b

The  ratio is I = 0.2545I_o

Explanation:

a

 From the question we are told that

        The wavelength is  \lambda = 600 nm

        The distance between the slit is  d = 0.117mm = 0.117 *10^{-3} m

        The width of the slit is  a = 35.7 \mu m = 35.7 *10^{-6}m

let  z be the number of fringes that appear between the first diffraction-envelope minima to either side of the central maximum in a double-slit pattern is  and this mathematically represented as

             z = \frac{d}{a}

Substituting values

             z = \frac{0.117*10^{-3}}{35.7 *10^{-6}}  

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b

   From the question  we are told that the order  of the bright fringe is  n = 3

   Generally the intensity of  a pattern  is mathematically represented as

                 I = I_o cos^2 [\frac{\pi d sin \theta}{\lambda} ][\frac{sin (\pi a sin \frac{\theta}{\lambda } )}{\pi a sin \frac{\theta}{\lambda} } ]

Where I_o is the intensity  of the  central fringe

 And  Generally  sin \theta = \frac{n \lambda }{d}

               I = I_o co^2 [ \frac{\pi (\frac{n \lambda}{d} )}{\lambda} ] [\frac{\frac{sin (\pi a (\frac{n \lambda}{d} ))}{\lambda} }{\frac{\pi a (\frac{n \lambda}{d} )}{\lambda} } ]

               I = I_o cos^2 (n \pi)[\frac{\frac{sin(\pi a (\frac{n \lambda}{d} ))}{\lambda} )}{ \frac{ \pi a (\frac{n \lambda }{d} )}{\lambda} } ]

               I = I_o cos^2 (3 \pi) [\frac{sin (\frac{3 \pi }{6} )}{\frac{3 \pi}{6} } ]

                I = I_o (1)(0.2545)

                  I = 0.2545I_o

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