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Diffraction by N-slits. Optical disturbance due to N slits.

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Presentation on theme: "Diffraction by N-slits. Optical disturbance due to N slits."— Presentation transcript:

1 Diffraction by N-slits

2 Optical disturbance due to N slits

3 Contribution of j th slit

4 Contribution of N slits

5 Irradiance due to N-slits I 0 = I rradiance by single slit at  =0

6 For principal maxima or

7 For minima Between consecutive principal maxima, there will be N-1 minima

8 Subsidiary maxima (N-2) subsidiary maxima between consecutive principle maxima

9 For large N, irradiance of first subsidiary maxima

10 Diffraction from multiple slits Slit Diffraction Pattern

11 Normal incidence Transmission grating

12 Oblique incidence a

13 For two wavelengths

14 Dispersive power of grating Width of principal maxima

15 Barely resolved ItIt  s  w

16 Chromatic resolving power of a grating

17 Chromatic resolving power of a prism

18

19 Reflection grating

20 Diffraction grating

21 The nominal track separation on a CD is 1.6 micrometers, corresponding to about 625 tracks per millimeter. This is in the range of ordinary laboratory diffraction gratings. For red light of wavelength 600 nm, this would give a first order diffraction maximum at about 22°.

22 15  15  0 nm 450 nm Atomic Force Microscope Image of CD

23 Bragg’s law X-ray diffraction from crystals: 2d Sin θ = n λ

24 Phase grating Delta function Bessel function

25 Problem Consider a opaque screen with 5 equally spaced narrow slits (spacing between them is d) and with monochromatic plane wave (wavelength ) incident normally. Draw a sketch of the transmitted intensity vs. angle to the normal for  = 0 to  = 1/5 radian. Take Sin  =  over this range and assume d/ =10. What is the ratio of least intense to the most intense peak? What is the angular distance of the first intense peak away from  = 0.


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