Class 33: Outline. Hour 1: Interference. Hour 2: Experiment 13: Interference P33-

Transcription

1 Class 33: Outline Hour 1: Interference Hour 2: Experiment 13: Interference P33-1

2 Last time: Microwaves (mw) c f = Hz λ = = 15cm mw mw f This time: Visible (red) light: c = = = f 14 Hz λ 5 cm red red f How in the world do we measure 1/10,000 of a cm? P33-2

3 We Use Interference This is also how we know that light is a wave phenomena P33-3

4 Interference: The difference between waves and bullets No Interference: if light were made up of bullets Interference: If light is a wave we see spreading and addition and subtraction P33-4

5 Interference: The difference between waves and bullets ons/light/08-waves2d/08-waves320.html P33-5

6 Interference Interference: Combination of two or more waves to form composite wave use superposition principle. Waves can add constructively or destructively Conditions for interference: 1. Coherence: the sources must maintain a constant phase with respect to each other 2. Monochromaticity: the sources consist of waves of a single wavelength P33-6

7 Demonstration: Microwave Interference P33-7

8 Interference Phase Shift Consider two traveling waves, moving through space: Look here as function of time Constructive Interference Look here as function of time Destructive Interference P33-8

9 Microwave Interference P33-9

10 Interference Phase Shift What can introduce a phase shift? 1. From different, out of phase sources 2. Sources in phase, but travel different distances 1. Thin films 2. Microwave Demonstration 3. Double-slit or Diffraction grating P33-10

11 PRS Question: Interference P33-11

12 Extra Path Length L In Phase Here Still in Phase Here L = mλ (m=0, ±1, ±2 ) Constructive Interference P33-12

13 Extra Path Length L In Phase Here Not in Phase Here ( 1 ) 2 L= m+ λ (m=0, ±1, ±2 ) Destructive Interference P33-13

14 Thin Film Interference - Iridescence Image courtesy of John M. Sullivan, University of Illinois and Technical University of Berlin. P33-14

15 Thin Film Interference - Iridescence Bubbles Butterfly Wings Oil on Puddles P33-15

16 Thin Film: Extra Path Extra path length ~ 2d 2d = mλ Constructive 2d = m+ λ Destructive d ( 1 ) 2 Oil on concrete, non-reflective coating on glass, etc. P33-16

17 Phase Shift = Extra Path? What is exact relationship between L & φ? sin( k x+ L ) = sin( kx+ k L) ( ) 2π = sin( kx + L) sin( kx + ϕ) λ L φ λ = 1 m constructive 2 π = m + 2 destructive P33-17

18 Two Transmitters P33-18

19 Microwave Interference P33-19

20 Two In-Phase Sources: Geometry Assuming δ = d sin L ( θ) d Extra path length : Assume L d λ y = Ltanθ L sin θ δ = dsin θ = mλ δ = dsin θ = + λ ( ) ( ) ( m 1 ) 2 Constructive Destructive P33-20

21 Interference for Two Sources in Phase (1) Constructive: (2) Destructive: δ = ( m + 1/2) λ 1 λl ydestructive = m+ m= 2 d δ = δ mλ sinθ = = = d d L λl yconstructive = m m= d 0,1,... mλ yconstructive 0,1... P33-21

22 In-Class: Lecture Demo Just Found: 1 λl ydestructive = m+ m= 0,1,... 2 d For m = 0 (the first minimum): y destructive = λ L 2d From our lecture demo, we measure: L ~ 1.16 m; d ~ 0.24 m; y destructive ~? m Estimate the wavelength & frequency of our microwaves P33-22

23 How we measure 1/10,000 of a cm Question: How do you measure the wavelength of light? Answer: Do the same experiment we just did (with light) First y destructive = λ L 2d λ is smaller by 10,000 times. But d can be smaller (0.1 mm instead of 0.24 m) So y will only be 10 times smaller still measurable P33-23

24 The Light Equivalent: Two Slits P33-24

25 Young s Double-Slit Experiment Bright Fringes: Constructive interference Dark Fringes: Destructive interference P33-25

26 PRS Question Double Slit Path Difference P33-26

27 Lecture Demonstration: Double Slit P33-27

28 Diffraction P33-28

29 Diffraction Diffraction: The bending of waves as they pass by certain obstacles No Diffraction No spreading after passing though slits Diffraction Spreading after passing though slits P33-29

30 Single-Slit Diffraction Derivation (Motivation) by Division: Divide slit into two portions: a δ = r1 r3 = r2 r4 = sinθ 2 Destructive interference: a ( 1 δ = sinθ = m + ) 2 λ 2 asinθ = mλ m=± 1, ± 2,... Don t get confused this is DESTRUCTIVE! P33-30

31 Intensity Distribution Destructive Interference: asinθ = mλ m=± 1, ± 2,... P33-31

32 Putting it Together P33-32

33 PRS Question: Two Slits with Width P33-33

34 Two Slits With Finite Width a With more than one slit having finite width a, we must consider 1. Diffraction due to the individual slit 2. Interference of waves from different slits P33-34

35 Two Slits With Finite width a Zero Order Maximum First Diff. Minimum a sinθ = λ First Order Maximum d sinθ = λ P33-35

36 Lecture Demonstration: Double Slits with Width P33-36

37 Babinet s Principle Case I: Put in a slit, get diffraction Case II: Fill up slit, get nothing Case III: Remove slit, get diffraction By superposition, the E field with the slit and the E field with just the filling must be exact opposites in order to cancel: E filling = E slit So the intensities are identical: I filling = I slit P33-37

38 Experiment 13: To Do Download Excel File! 1. Single Slit 4 different slits. Use known width a and zeroes y destructive to Estimate wavelength of red light 2. Human Hair (Babinet says just single slit). Use λ red (from 1) and zeroes y destructive to Estimate thickness of hair 3. Double Slit 4 different slits. Use known spacing d and zeroes to Estimate wavelength of red light 4. CD Track Spacing (Diffraction Grating) Estimate track spacing P33-38