Transcript Chapter 35
Chapter 37 Interference of Light Waves (Cont.) PHY 1371 Dr. Jie Zou 1 Outline Change of phase due to reflection Lloyd’s mirror Phase change due to reflection Interference in thin films Interference in a wedge-shaped film Newton’s rings PHY 1371 Dr. Jie Zou 2 Lloyd’s Mirror Lloyd’s mirror: Another simple, yet ingenious, arrangement for producing an interference pattern with a single light source. Observation: Lloyd’s Mirror PHY 1371 An interference pattern is observed on the viewing screen. However, the positions of the dark and bright fringes are reversed relative to the pattern created by Young’s experiment. Dr. Jie Zou 3 Change of phase due to reflection PHY 1371 Explanation for the previous observation: The coherent light sources at points S and S’ differ in phase by 180° (or rad), a phase change produced by reflection. In general, an electromagnetic wave undergoes a phase change of 180° upon reflection from a medium that has a higher index of refraction than the one in which the wave is traveling. Dr. Jie Zou 4 An analogy The general rules: An electromagnetic wave undergoes a 180° phase change when reflected from a boundary leading to an optically denser (larger n) medium. No phase change occurs when the electromagnetic wave is reflected from a boundary leading to a less optically dense (smaller n) medium. PHY 1371 Dr. Jie Zou 5 Observation of interference effects in thin films PHY 1371 Examples of thin films in everyday life: thin layers of oil on water or the thin surface of a soap bubble. Observation: varied colors are observed when white light is incident on such thin films. Explanation for the observation: The varied colors result from the interference of waves reflected from the two surfaces of the film. Dr. Jie Zou 6 Interference in thin films Two factors should be considered: 1. 2. PHY 1371 The difference in path length for the two rays. The 180° phase change upon reflection. Assumption: Normal incidence. Condition for constructive interference: 2nt = (m+1/2), m =0, 1, 2… Condition for destructive interference: 2nt = m, m = 0, 1, 2… Note: These conditions are true only when n1<n>n2 or n1>n<n2,, when a net phase change of 180° due to reflection occurs. Dr. Jie Zou 7 Example 37.5: Interference in a wedge-shaped film PHY 1371 A thin, wedge-shaped film of refractive index n is illuminated with monochromatic light of wavelength . Describe the interference pattern observed for this case. Dr. Jie Zou 8 Example 37.4 Nonreflective coatings for solar cells PHY 1371 Suppose that a silicon (si) solar cell (n = 3.5) is coated with a thin film of silicon monoxide (SiO, n= 1.45) in order to minimize reflective losses from the surface. Find the minimum film thickness that produces the least reflection at a wavelength of 550 nm, near the center of the visible spectrum. Dr. Jie Zou 9 Newton’s rings Set up: A plano-convex lens on top of a flat glass surface. PHY 1371 The air film between the glass surfaces varies in thickness. Observation: A pattern of light and dark rings when observed from above using light of a single wavelength. Derivation for the radii of the dark rings (Problem #67): rm (mR/nfilm)1/2, m =0, 1, 2… Dr. Jie Zou 10 Homework Ch. 37, P. 1200, Problems: #32, 33, 39, 62. PHY 1371 Dr. Jie Zou 11