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Double Slit Interference. Intensity of Double Slit E= E 1 + E 2 I= E 2 = E 1 2 + E 2 2 + 2 E 1 E 2 = I 1 + I 2 + “interference” <== vanishes if incoherent.

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Presentation on theme: "Double Slit Interference. Intensity of Double Slit E= E 1 + E 2 I= E 2 = E 1 2 + E 2 2 + 2 E 1 E 2 = I 1 + I 2 + “interference” <== vanishes if incoherent."— Presentation transcript:

1 Double Slit Interference

2 Intensity of Double Slit E= E 1 + E 2 I= E 2 = E 1 2 + E 2 2 + 2 E 1 E 2 = I 1 + I 2 + “interference” <== vanishes if incoherent

3 Refraction In general v = f and changes if v does in vacuum c = f in a medium c/n = n f hence n = /n which is less than consider two light waves which are in phase in air (n=1) and each passes through a thickness L of different material upper wave has 2 = /n 2 lower wave has 1 = /n 1

4 Refraction Wave 2 has N 2 = L/ 2 = (L/ )n 2 wavelengths in block Wave 1 has N 1 = L/ 1 = (L/ )n 1 wavelengths in block hence N 2 -N 1 = (L/ )(n 2 -n 1 ) phase change of wave 1 is k 1 x-  t (2  / 1 )L -  t phase change of wave 2 is k 2 x-  t (2  / 2 )L -  t phase difference =(2  L/ )(n 2 -n 1 ) = 2  (N 2 -N 1 )

5 Refraction Emerging waves are out of phase interfere constructively if phase difference is 2  x integer (2  L/ )(n 2 -n 1 ) = 2  m hence L = m /(n 2 -n 1 )

6 Problem Which pulse travels through the plastic in less time?

7 Solution t=d/v pulse 2: t=t 1 +t 2 +t 3 +t 4 v 1 =c/1.55, v 2 =c/1.70, v 3 =c/1.60, v 4 =c/1.45 t=(L/c)( 1.55+1.70+1.60+1.45)=6.30(L/c) pulse 1: t= t 1 +t 2 +t 3 v 1 =c/1.59, v 2 =c/1.65, v 3 =c/1.50 t=(L/c)(2 x 1.59 + 1.65 +1.50)=6.33(L/c) pulse 2 takes least time

8 Phase Change due to Reflection Soap films, oil slicks show interference effects of light reflected from the top and bottom surfaces When a wave moves from one medium to another there is a phase shift of  if it moves more slowly in the second medium and zero if it moves more quickly Why does top portion of film appear dark? Why are there different colours?

9 Fixed End Phase change of 

10 Free End No phase change

11 What is phase difference between rays 1 and 2 ? ray 2 travels further => phase difference due to path difference phase difference due to extra thickness is (2  / `)(2t) but ` is the wavelength in the water medium! ` = /n ray 1 is reflected from a medium with slower speed ray 2 is reflected from a medium with higher speed extra phase difference of  due to reflection of ray 1 total phase difference  =  + (2  n/ )(2t)

12 Both rays reflected from media in which wave moves more slowly phase difference only due to path difference  = (2  n water / )(2t) if  = 2  m, then constructive interference if  =  (2m-1), then destructive interference  = (2  n water / )(2t) =  (2m-1), i.e. t = (2m-1)( /4n water ) non-reflecting glass uses this principle

13 1. Find d for the 19th and 20th bright fringe: path difference? black ray travels extra distance 2d in air =>phase diff = (2  / )(2d) note: n=1! black ray has extra phase difference of  due to reflection bright fringe when  = (2  / )(2d)+  =2  m => d=(m-1/2)( /2) 2. Give the limits on d d 19 = (19 – 1/2) /2 = 5457 nm; d 20 = 5753 nm hence 5.46 µm < d < 5.75 µm The diameters of fine wires can be accurately measured using interference patterns. Two optically flat pieces of glass of length L are arranged with the wire between them as shown above. The setup is illuminated by monochromatic light, and the resulting interference fringes are detected. Suppose L = 20 cm and yellow sodium light (  590 nm) is used for illumination. If 19 bright fringes are seen along this 20-cm distance, what are the limits on the diameter of the wire? Hint: The nineteenth fringe might not be right at the end, but you do not see a twentieth fringe at all.

14 Newton’s Rings Light reflected from curved lens interferes with lift reflected from plate: bright ring  =  + (2  / )(2d)=2m  2d=(m-1/2) max


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