diffraction physics 202 professor lee carkner lecture 26
Post on 21-Dec-2015
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PAL #25 Interference Applications
Wavelength of laser D = d = 0.25 mm = 0.00025 m y = 1.5 cm = 0.015 m (between any 2
maxima) = yd/D = (0.015)(2.5X10-4)/(5.5) = 682 nm
Is this reasonable?
Diffraction When light passes though a small aperture it
spreads out
This effect also occurs when light passes by an obstacle
The pattern consists of minima and maxima of decreasing intensity as you move away from the center
Diffraction and Optics
Real point sources of light always experience diffraction and so we never see true point images
Diffraction limits even the best optics
Degree of diffraction (and blurriness) depends on aperture size and wavelength
Diffraction and Interference
Light rays from different parts of the same aperture can also produce interference
Instead of two rays from two slits, we have a continuum of rays emerging from one slit
Path Length Difference Minima (dark fringes) should occur at the point where
half of the rays are out of phase with the other half
If we assume that the distance to the screen (D) is much larger than the slit width (a) then the path difference is
where d is the distance between the origin points of the two
rays
We will pair up the rays, and find the path length for which each pair cancels out
Location of the Minima Since:
L /d = sin
How far apart can a pair of rays get?
For the first minima L must equal /2:
a sin =
Diffraction Patterns Since a sin = for m=1, we can say for the more
general case:a sin = m(min)
The maxima are located halfway between the minima
Since waves from the top and bottom half cancel
Smaller slit means more flaring
Intensity
Intensity of maxima decrease with increasing
We will use which is half the phase difference between the top and bottom of the slit
= ½ = (a/) sin I = Im (sin /)2
Intensity Variations The intensity falls off rapidly with linear
distance y Remember tan = y/D
The narrower the slit the broader the maximum Remember:
m = 1.5, 2.5, 3.5 … maxima
Diffraction and Circular Apertures
The location of the minima depend on the wavelength and the diameter instead of slit width:
For m = 1
The minima and maxima appear as concentric circles
Resolution Since virtually all imaging devices
have apertures, virtually all images are blurry
If you view two point sources that are very close together, you may not be able to distinguish them