Lecture 27B - UCSD Department of Physics
Transcription
Lecture 27B - UCSD Department of Physics
Physics 1C Lecture 27B “Think left and think right and think low and think high. Oh, the thinks you can think up if only you try! Dr. Seuss http://www.microscopyuk.org.uk/mag/indexmag.html?http://www.microscopyuk.org.uk/mag/artmay08/mm-bubbles.html Quiz 3 Info Next Wednesday It will be a Scantron test that covers Chapters 24, 25, and 26. A list of equations, constants, and conversions will be provided on the quiz. Outline Last Time Interference, double slit, thin films Today CD/DVD Thin film interference Single slit diffraction Resolution Compact Disk (CD) y = Ll/d = (1 m)(6.6 x 10-7 m)/(1.6 x 10-6 m) y = 0.42 m Clicker Question 27B-1 What is the approximate spacing between DVD tracks if the distance between the DVD and screen needs to be adjusted to approximately one-half to match the first order peaks position? A. The same B. Approximately half C. Approximately double D. Approximately one-quarter E. Approximately quadruple DVD y = Ll/d If LDVD ~ 0.4 x LCD for the same y, what is d ?? d = 0.65 mm = (0.65 x 10-6 m) But how is a CD read? Diffraction can separate Colors Interference and Reading CDs Optical Engineering Interference in Thin Films Interference in soap bubbles. The colors are due to interference between light rays reflected from the front and back surfaces of the thin film of soap making the bubble. The color depends on the thickness of the film. Black appears where the film is thinnest. Red appears where the film is thickest. Interference in Thin Films A light wave will undergo a phase change of 180o upon reflection from a medium of higher index of refraction than the one in which it was traveling. So, an electromagnetic wave traveling in air will undergo a 180o phase shift if it reflects off an oil surface. This is similar to the reflection of a transverse wave that we observed earlier off of a rigid surface. Interference in Thin Films A light wave will not undergo a phase change upon reflection from a medium of lower index of refraction than the one in which it was traveling. So, a light wave traveling in oil will not undergo a phase shift if it reflects off an air boundary. This is similar to the reflection of a transverse wave that we observed earlier off of a free surface. Interference in Thin Films With light incident on a thin film we have to examine two light rays that follow the same path: Ray 1 (in air) reflects off the film surface and undergoes a phase change of 180o compared to the incident ray. Ray 2 (in air) refracts at the film surface and then reflects off of Surface B (film to air) with no phase change compared to the incident wave. Interference in Thin Films In addition, Ray 2 travels a distance t down and and a distance t up (for a total distance 2t). Since the extra distance that Ray 2 travels is in the film medium, its wavelength will be different then in air. The wavelength of light, λn, in a medium with index of refraction n is: l ln where λ is wavelength of light in a vacuum (air?). n Interference in Thin Films In order for constructive interference to occur, the two rays must be in phase. This means that the difference in path length and phase must combine to m(λ / n), where m = 0, ±1, ±2... The difference in path is: 2t and the difference in phase is: 1 l 2 n Combining all of these gives us: 1l l 2t m 2n n 2nt m l 1 2 Constructive Interference for 1 phase change. Interference in Thin Films With light incident on a thin film with another thin film of higher index of refraction below the first: Ray 1 (in air) reflects off the film surface and undergoes a phase change of 180o compared to the incident ray. Ray 2 (in 1st film) reflects off the film surface and undergoes a phase change of 180o compared to the incident ray. Thin Film Interference To solve thin film interference problems you have to know how many phase reversals there are. Then you know which equation to use: Equation 1 phase reversal 0 or 2 phase reversals 2nt = (m+1/2)λ constructive destructive 2nt = mλ destructive constructive Thin Film Interference Thin Film Interference Problem Solving Strategy: 1) Identify the thin film causing the interference. 2) Determine the indices of refraction in the film and the media on either side of it. 3) Determine the number of phase reversals: zero, one or two. 4) If the interference is constructive with 0 or 2 phase reversal then use a path length difference of integral multiples of λ (use odd half multiple of λ for 1 phase reversal). Clicker Question 27B-2 Upon reflection, light undergoes a 180o phase change: A) If the incident medium has the lower index of refraction B) Never C) Whenever the incident angle is less than the critical angle D) Always E) If the incident medium has the higher index of refraction (N.B.: Incident medium is the medium where both incident and reflected waves are propagating) Thin Film Interference 5) If the interference is destructive with 0 or 2 phase reversal then use a path length difference of odd half multiples of λ (use integral multiple of λ for 1 phase reversal). Thin film interference is used by Morpho butterflies to intensify the colors reflected: . structural color or iridescence Thin Film Interference Can be observed in a more continuous manner in Mellon jelleyfish Cilia beat in pulses to propel the jellyfish through the water. The cilia are so close together that they cause interference The varying distances between the cilia during pulsing producing a range of colors Bio-Layer Interferometry (BLI) • • • Much studied physical principle commonly use in surface profiling, semiconductor industry, astrophysics Optical layer reflects simple white light; second reflection from tip of biosensor, both reach detector Analyte binding changes thickness of bio-layer, which is measured at detector Diffraction Patterns The diffraction pattern that appears on a screen when light passes through a narrow vertical slit. The pattern consists of a broad, intense central band and a series of less intense and narrower side bands. A diffraction pattern is actually a misnomer. In reality it is another interference pattern. Diffraction Patterns Diffraction pattern of a penny, taken with the penny midway between screen and source. The shadow of a penny displays bright and dark rings of a diffraction pattern. The bright center spot is called the Arago bright spot. The bright spot is explained by the wave theory of light. Waves that diffract on the edges of the penny all travel the same distance to the center. The center is a point of constructive interference Single Slit Experiment A single slit of a finite width placed between a distant light source and a screen produces a diffraction pattern (similar to a double slit experiment). It will have a broad, intense central band. The central band will be flanked by a series of narrower, less intense secondary bands (secondary maxima) that form the diffraction pattern. Single Slit Experiment The bright central band of the pattern will also be flanked by a series of dark bands (minima). In general, destructive interference occurs for a single slit of width, a, when: ml sin a where m is ±1, ±2, ±3... You can observe the at the first minimum angle: l sin 1 a Action figure Single Slit Experiment The cause of single slit interference is path length difference (just like double slit interference). In the single slit case, 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 of the slit. You can again use the approximation: y sin L For Next Time (FNT) Finish reading Chapter 27 Continue working on homework for Chapter 27