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Introduction to SAT II Physics - FreeExamPapers

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Note that the pattern is brightest in the middle, where = 0. This point is called the<br />

central maximum. If you encounter a question regarding double-slit refraction on the<br />

test, you’ll most likely be asked <strong>to</strong> calculate the distance x between the central maximum<br />

and the next band of light on the screen. This distance, for reasons <strong>to</strong>o involved <strong>to</strong><br />

address here, is a function of the light’s wavelength ( ), the distance between the two<br />

slits (d), and the distance between the two screens (L):<br />

Diffraction<br />

Diffraction is the bending of light around obstacles: it causes interference patterns such<br />

as the one we saw in Young’s double-slit experiment. A diffraction grating is a screen<br />

with a bunch of parallel slits, each spaced a distance d apart. The analysis is exactly the<br />

same as in the double-slit case: there are still maxima at d sin = n and minima at d sin<br />

= (n + 1/2) . The only difference is that the pattern doesn’t fade out as quickly on the<br />

sides.<br />

Single-Slit Diffraction<br />

You may also find single-slit diffraction on <strong>SAT</strong> <strong>II</strong> <strong>Physics</strong>. The setup is the same as with<br />

the double-slit experiment, only with just one slit. This time, we define d as the width of<br />

the slit and as the angle between the middle of the slit and a point P.<br />

Actually, there are a lot of different paths that light can take <strong>to</strong> P—there is a path from<br />

any point in the slit. So really, the diffraction pattern is caused by the superposition of an<br />

infinite number of waves. However, paths coming from the two edges of the slit, since<br />

they are the farthest apart, have the biggest difference in phase, so we only have <strong>to</strong><br />

consider these points <strong>to</strong> find the maxima and the minima.<br />

Single-slit diffraction is nowhere near as noticeable as double-slit interference. The<br />

maximum at n = 0 is very bright, but all of the other maxima are barely noticeable. For<br />

this reason, we didn’t have <strong>to</strong> worry about the diffraction caused by both slits individually<br />

when considering Young’s experiment.<br />

Polarization<br />

309

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