Physics 102: Lecture 20 Interference 1.

Slides:



Advertisements
Similar presentations
The Wave Nature of Light Thin Film Interference
Advertisements

Waves (in general) sine waves are nice
PH 103 Dr. Cecilia Vogel Lecture 8. Review Outline  diffraction  interference  coherence  Diffraction/interference examples  double - slit and diffraction.
AP Physics Mr. Jean March 30 th, The plan: Review of slit patterns & interference of light particles. Quest Assignment #2 Polarizer More interference.
Physics 6C Interference of EM Waves Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Chapter 34 The Wave Nature of Light; Interference
Interference Physics 202 Professor Lee Carkner Lecture 22.
Phys 102 – Lecture 22 Interference 1. Physics 102 lectures on light Lecture 15 – EM waves Lecture 16 – Polarization Lecture 22 & 23 – Interference & diffraction.
Textbook sections Physics 1161: Pre-Lecture 26 Interference.
Physics 1402: Lecture 33 Today’s Agenda Announcements: –Midterm 2: graded after Thanks Giving –Homework 09: Friday December 4 Optics –interference.
Physics 52 - Heat and Optics Dr. Joseph F. Becker Physics Department San Jose State University © 2005 J. F. Becker.
Chapter 25: Interference and Diffraction
Diffraction, Gratings, Resolving Power
Physics 1161: Lecture 20 Interference textbook sections
3: Interference, Diffraction and Polarization
Lecture 15 Interference Chp. 35
Physics 6C Interference of EM Waves. Young’s Double Slit Experiment In Young’s double-slit experiment light comes from the left and passes through the.
Lecture 15 Interference Chp. 35 Topics –Interference from thin films –Due to the wave nature of light –Change in wavelength and phase change in a medium.
Chapter 27 Interference and the Wave Nature of Light.
Interference and the Wave Nature of Light
Textbook sections Physics 1161: Lecture 26 Interference.
CHAPTER 37 : INTERFERENCE OF LIGHT WAVES
Chapter 27 Interference and the Wave Nature of Light.
Thursday, Sep. 4Phy208 Lecture 2 1 From last time… Waves Interference Please pick up pack of color sheets.
Thus, the image formed by lens 2 is located 30 cm to the left of lens 2. It is virtual (since i 2 < 0). 30 The magnification is m = (-i 1 /p 1 ) x (-i.
Diffraction is the bending of waves around obstacles or the edges of an opening. Huygen’s Principle - Every point on a wave front acts as a source of tiny.
S-110 A.What does the term Interference mean when applied to waves? B.Describe what you think would happened when light interferes constructively. C.Describe.
Interference Applications Physics 202 Professor Lee Carkner Lecture 25.
Light Interference Continued…
Ch 16 Interference. Diffraction is the bending of waves around obstacles or the edges of an opening. Huygen’s Principle - Every point on a wave front.
Agenda Today –Thin Film Interference Friday –Diffraction (Ch. 36)
Physics 11 Advanced Mr. Jean May 23 rd, The plan: Video clip of the day Wave Interference patterns Index of refraction Slit & Double Slit interference.
Physics 102: Lecture 19, Slide 1 Today’s Lecture will cover textbook sections 23.9, 24.1, 3-4, 6 Physics 102: Lecture 19 Lenses and your EYE Ciliary Muscles.
Thin Film Interference Interference + Light. Superposition t +1 t +1 t Destructive Interference Out of Phase 180 degrees.
Physics 102: Lecture 20 Interference 1.
Chapter 24: Young’s Experiment Llyod’s Mirror Thin Films.
Chapter 24 The Wave Nature of Light
Young’s Double Slit Contents: Interference Diffraction Young’s Double Slit Angle Distance.
Thursday, Sep. 4Phy208 Lecture 2 1 From last time… Waves Interference Please pick up pack of color sheets.
Thin Film Interference Interference + Light. Superposition t +1 t +1 t Destructive Interference Out of Phase 180 degrees.
Today’s Lecture will cover textbook sections 23.9,24.1,3-4,6 Physics 102: Lecture 19 Lenses and your EYE Ciliary Muscles.
Physics 102: Lecture 21, Slide 1 Diffraction, Gratings, Resolving Power Physics 102: Lecture 21.
Physics 102: Lecture 20, Slide 1 Hour Exam 3 Monday, Apr. 18 (two weeks from today!) –Lectures 14 – 21 –Homework through HW 11 –Discussions through Disc.
PHYS219 Fall semester 2014 Lecture 23: Wave Nature of Light: Thin Film Interference and Diffraction Gratings Dimitrios Giannios Purdue University.
Advanced Higher Physics Interference
Interference & Diffraction
Ch 16 Interference.
Diffraction, Gratings, Resolving Power
Interference.
Geometry of Young’s Double Slit Experiment
Diffraction, Gratings, Resolving Power
Interference Principle of Superposition- Constructive Interference
Physics 102: Lecture 19 Lenses and your EYE Ciliary Muscles 1.
Physics 102: Lecture 20 Interference 1.
Interference of EM Waves
Physics 102: Lecture 19 Lenses and your EYE Ciliary Muscles 1.
Diffraction and Thin Film Interference
Interference and the Wave Nature of Light
Light Interference Continued…
Phys102 Lecture 25 The Wave Nature of Light; Interference
A –Level Physics: Waves and Quanta: Wave Phase and Interference
Phys102 Lecture 25 The Wave Nature of Light; Interference
Physics 1B03summer-Lecture 11
Diffraction, Gratings, Resolving Power
Physics 1161: Lecture 19 Lenses and your EYE
Interference.
Diffraction, Gratings, Resolving Power
The Geometry of Interference and Diffraction
Physics 102: Lecture 20 Interference 1.
Reflection and Refraction of Light
Presentation transcript:

Physics 102: Lecture 20 Interference 1

Unaided Eye Bring object as close as possible (to near point dnear) How big the object looks with unaided eye. object h0 q dnear Bring object as close as possible (to near point dnear) **If q is small and expressed in radians.

Angular Size Preflight 19.6, 19.7 Both are same size, but nearer one looks bigger. q q q q Angular size tells you how large the image is on your retina, and how big it appears to be. How small of font can you read? Highwire Caramel Apples Rabbits Kindergarten Hello Arboretum Halloween Amazing

Magnifying Glass object virtual image hi ho di do magnifying glass Magnifying glass produces virtual image behind object, allowing you to bring object to a closer do: and larger q′ Compare to unaided eye: : Ratio of the two angles is the angular magnification M:

Angular Magnification magnifying glass virtual image object (dnear = near point distance from eye.) hi ho do di For the lens : 1 d o + i = f Þ - For max. magnification, put image at dnear: so set di = -dnear: M = dnear /d0 = dnear/f +1 Smaller f means larger magnification

Constructive Interference Superposition Constructive Interference t +1 -1 + t +1 -1 In Phase t +2 -2

Destructive Interference Superposition Destructive Interference +1 t -1 + +1 Out of Phase 180 degrees t -1 t +2 -2

Superposition ACT + Different f 1) Constructive 2) Destructive 3) Neither

Interference Requirements Need two (or more) waves Must have same frequency Must be coherent (i.e. waves must have definite phase relation)

Interference for Sound … For example, a pair of speakers, driven in phase, producing a tone of a single f and l: hmmm… I’m just far enough away that l2-l1=l/2, and I hear no sound at all! l1 l2 Demo 440 Sound Interference But this won’t work for light--can’t get coherent sources

Interference for Light … Can’t produce coherent light from separate sources. (f  1014 Hz) Need two waves from single source taking two different paths Two slits Reflection (thin films) Diffraction* Single source Two different paths Interference possible here

ACT: Young’s Double Slit Light waves from a single source travel through 2 slits before meeting on a screen. The interference will be: Constructive Destructive Depends on L d Single source of monochromatic light  L 2 slits-separated by d Screen a distance L from slits

Preflight 20.1 The experiment is modified so that one of the waves has its phase shifted by ½ l. Now, the interference will be: Constructive Destructive Depends on L ½ l shift d The rays start out of phase, and travel the same distance, so they will arrive out of phase. 60% got this correct Single source of monochromatic light  L 2 slits-separated by d Screen a distance L from slits

Young’s Double Slit Concept At points where the difference in path length is 0, l,2l, …, the screen is bright. (constructive) 2 slits-separated by d d At points where the difference in path length is the screen is dark. (destructive) Demo 162 2 slit Single source of monochromatic light  L Screen a distance L from slits

Young’s Double Slit Key Idea Two rays travel almost exactly the same distance. (screen must be very far away: L >> d) Bottom ray travels a little further. Key for interference is this small extra distance.

Young’s Double Slit Quantitative Path length difference = d sin q Constructive interference ______________ Destructive interference _______________ Need l < d where m = 0, or 1, or 2, ...

Young’s Double Slit Quantitative A little geometry… sin(q)  tan(q) = y/L Constructive interference Destructive interference where m = 0, or 1, or 2, ... 33

Preflight 20.3 L y d When this Young’s double slit experiment is placed under water. The separation y between minima and maxima 1) increases 2) same 3) decreases

Preflight 20.2 In the Young double slit experiment, is it possible to see interference maxima when the distance between slits is smaller than the wavelength of light? 1) Yes 2) No

Thin Film Interference 1 2 n0=1.0 (air) n1 (thin film) t n2 Demo 70 soap film Get two waves by reflection off two different interfaces. Ray 2 travels approximately 2t further than ray 1.

Reflection + Phase Shifts Incident wave Reflected wave n1 n2 Upon reflection from a boundary between two transparent materials, the phase of the reflected light may change. If n1 > n2 - no phase change upon reflection. If n1 < n2 - phase change of 180º upon reflection. (equivalent to the wave shifting by l/2.)

Note: this is wavelength in film! (lfilm= lo/n1) Thin Film Summary Determine d, number of extra wavelengths for each ray. 1 2 n = 1.0 (air) n1 (thin film) t n2 This is important! Note: this is wavelength in film! (lfilm= lo/n1) Reflection Distance Ray 1: d1 = 0 or ½ + 0 Ray 2: d2 = 0 or ½ + 2 t/ lfilm If |(d2 – d1)| = 0, 1, 2, 3 …. (m) constructive If |(d2 – d1)| = ½ , 1 ½, 2 ½ …. (m + ½) destructive

Thin Film Practice (ACT) Example 1 2 n = 1.0 (air) nglass = 1.5 t nwater= 1.3 Blue light (lo = 500 nm) incident on a glass (nglass = 1.5) cover slip (t = 167 nm) floating on top of water (nwater = 1.3). Is the interference constructive or destructive or neither? A) d1 = 0 B) d1 = ½ C) d1 = 1 What is d1, the total phase shift for ray 1

Thin Film Practice Example 1 2 n = 1.0 (air) nglass = 1.5 t nwater= 1.3 Blue light (lo = 500 nm) incident on a glass (nglass = 1.5) cover slip (t = 167 nm) floating on top of water (nwater = 1.3). Is the interference constructive or destructive or neither? d1 = Reflection at air-film interface only d2 = Phase shift = d2 – d1 =

ACT: Thin Film Blue light l = 500 nm incident on a thin film (t = 167 nm) of glass on top of plastic. The interference is: (A) constructive (B) destructive (C) neither 1 2 n=1 (air) nglass =1.5 t nplastic=1.8 Brian Dvorkin has had good luck with the following presentation. 1) Look for the ½ wavelength shifts on reflection. Then ask for constructive interference what do I need ray 2 to do? (0 or ½ wavelength more?) If choose 0, increase to 1. d1 = d2 = Phase shift =

Preflights 20.4, 20.5 t = l nwater=1.3 ngas=1.20 nair=1.0 noil=1.45 A thin film of gasoline (ngas=1.20) and a thin film of oil (noil=1.45) are floating on water (nwater=1.33). When the thickness of the two films is exactly one wavelength… The gas looks: bright dark The oil looks: bright dark