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Transcript
Chapter 38: Diffraction and
Polarization
 For a single opening in a barrier, we might
expect that a plane wave (light beam) would
produce a bright spot the same size as the open
However, what we actually see is a series of light
and dark fringes similar the double-slit interference
We call this a diffraction pattern
 We will only consider the case
where L is very large
 Fraunhofer diffraction
pattern
 For a screen close to the slit, a
Fresnel diffraction pattern is
created
 As for the double-slit problem, we
take L to be large so that the rays
from the slit are parallel
Consider slit width a
 Divide the slit into N
equally space zones of
width y. So, a=Ny
 Using Huygen’s principle,
we consider each zone to
be a point source emitting
spherical rays
 Each contributes an
electric field E at point P
on the screen
 The total electric field is
the resultant from all zones
Phasor diagrams
Example Problem 38.6
Light of wavelength 587.5 nm
illuminates a single slit 0.750 mm in
width. (a) At what distance from the slit
should a screen be located if the first
minimum in the diffraction pattern is to
be 0.850 mm from the center of the
principal maximum? (b) What is the
width of the central maximum?