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UK PHY 213 - Physics 213 General Physics

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Physics 213 General PhysicsExam 2PowerPoint PresentationInterference PatternsDiffractionDiffraction PatternSingle Slit DiffractionSingle Slit Diffraction, 2Single Slit Diffraction, 3Single Slit Diffraction, 4Slide 11Slide 12Diffraction GratingDiffraction Grating, finalPolarization of Light WavesPolarization of Light, contSlide 17Polarization by Selective AbsorptionPolarization by Scattering, contPhysics 213General PhysicsLecture 18Exam 2+12 additional points will be added to each score.3Last Meeting: InterferenceToday: Diffraction and PolarizationInterference PatternsConstructive interference occurs when waves arrive in phaseDiffractionHuygen’s principle requires that the waves spread out after they pass through slitsThis spreading out of light from its initial line of travel is called diffractionIn general, diffraction occurs when waves pass through small openings, around obstacles or by sharp edgesDiffraction PatternA single slit placed between a distant light source and a screen produces a diffraction patternIt will have a broad, intense central bandThe central band will be flanked by a series of narrower, less intense secondary bandsCalled secondary maximaThe central band will also be flanked by a series of dark bandsCalled minimaSingle Slit DiffractionAccording to Huygen’s principle, each portion of the slit acts as a source of wavesThe light from one portion of the slit can interfere with light from another portionThe resultant intensity on the screen depends on the direction θSingle Slit Diffraction, 2All the waves that originate at the slit are in phaseWave 1 travels farther than wave 3 by an amount equal to the path difference (a/2) sin θ If this path difference is exactly half of a wavelength, the two waves cancel each other and destructive interference resultsSingle Slit Diffraction, 3In general, destructive interference occurs for a single slit of width a when sin θdark = mλ / am = 1, 2, 3, …Doesn’t give any information about the variations in intensity along the screenSingle Slit Diffraction, 4The general features of the intensity distribution are shownA broad central bright fringe is flanked by much weaker bright fringes alternating with dark fringesThe points of constructive interference lie approximately halfway between the dark fringes11sin θdark = mλ / a m = 1, 2, 3, …sin θbright = mλ / d m =0  1, 2, 3, …There are two difficulties in using a double slit for measuring wavelengths. 1. The bright linesbright lines on the screen are actually extremely faintfaint and an intense light source is therefore required;2. The lines are relatively broad and it is hard to locate their center accurately.Diffraction GratingThe condition for maxima isd sin θbright = m λm = 0, 1, 2, …The integer m is the order number of the diffraction patternIf the incident radiation contains several wavelengths, each wavelength deviates through a specific angleDiffraction Grating, finalAll the wavelengths are focused at m = 0This is called the zeroth order maximumThe first order maximum corresponds to m = 1Note the sharpness of the principle maxima and the broad range of the dark areaThis is in contrast to the broad, bright fringes characteristic of the two-slit interference patternPolarization of Light WavesEach atom produces a wave with its own orientation of All directions of the electric field vector are equally possible and lie in a plane perpendicular to the direction of propagationThis is an unpolarized waveEPolarization of Light, contA wave is said to be linearly polarized if the resultant electric field vibrates in the same direction at all times at a particular pointPolarization can be obtained from an unpolarized beam by Selective absorptionReflectionScatteringExamples of Polarized LightPolarization by Selective AbsorptionThe most common technique for polarizing lightUses a material that transmits waves whose electric field vectors in the plane are parallel to a certain direction and absorbs waves whose electric field vectors are perpendicular to that directionE=E0cosI=I0cos2Polarization by Scattering, contThe horizontal part of the electric field vector in the incident wave causes the charges to vibrate horizontallyThe vertical part of the vector simultaneously causes them to vibrate verticallyHorizontally and vertically polarized waves are


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UK PHY 213 - Physics 213 General Physics

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