wave phenomena
DESCRIPTION
Wave Phenomena. Wu, Jinyuan Fermilab Aug. 2013. Introduction. We will talk about classical physics only. We will try to show phenomena not commonly seen in text book. Many pictures in this file are taken via www.google.com They are used for review and comments only. - PowerPoint PPT PresentationTRANSCRIPT
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Wave Phenomena
Wu, JinyuanFermilabAug. 2013
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 2
Introduction We will talk about classical physics only. We will try to show phenomena not commonly
seen in text book.
Many pictures in this file are taken via www.google.comThey are used for review and comments only.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 4
Repetitive Motions of many Things
We live in a world with two type of motions: One pass motions. Repetitive motions.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 5
Inertia and Recovery Force of Oscillations
An object needs two elements in order to oscillate: Recovery force: so that the object moves back and forth around an origin. Inertia: so that the object keeps moving.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 6
Boundary Conditions and Eigen Values
When an object is supported differently, the resonant frequencies can different.
Different boundary conditions causes different movement modes with different Eigen Values
“DO”
“SO”
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 7
Frequency vs. Length
F = const. x (1/L) Guitar Violin Organ
F = const. x (1/L)2
Xylophone
F ~ const. x (1/L)0
Rubber band string
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 8
Multi-wire Chambers (1)
When a charged particle passes through, the gas in the multi-wire chamber is ionized.
Electrons drift toward signal wires under electrical field generated by the high voltage wires.
When the electrons arrive the signal wires, electrical pulses are detected.
From arrival time, the track position can be determined.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 9
Multi-wire Chambers (2)
Several planes of multi-wire chambers can be used to determine the track direction.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 10
Straw Tube Chambers
The wire can be stretched in a plastic tube with metalized walls.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 11
Wire Tension Measurement
Wires must be stretched to certain tension to hold their positions. To measure the wire tension, a pulse of current is sent through the wire in a magnetic field. The resonant frequency is recorded to calculate the wire tension.
LmT
Lf
/21
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Reflection
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 13
Waves reflect at the boundary of two media.
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Retro-reflection (1) Animal Eyes
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 14
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Retro-reflection (2) Mirror Corner
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 15
Show the retro-reflectivity of the mirror corner. (using <10 lines)
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Retro-reflection (3) Glass Ball
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 16
a
b
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Glass Balls with Different n
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 17
When the index of refraction is ~2, most incident light will reflect back.
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Glass Ball Submerged in Water
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 18
When the glass ball is submerged in water, relative index of refraction becomes ~ 2/1.33 = 1.5
Most incident light will reflect away. The highway lane paint is difficult to see in rainy nights.
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Impedance Mismatch & Optical Reflection
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 20
The reflection seen above is due to difference of the impedances (not index of refraction!) of media.
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Acoustic Impedance Mismatch for Muffler
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 21
ImpedanceMismatch
ImpedanceMismatchImpedanceMismatch
ImpedanceMismatch
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 22
Sound Wave Reflection at the Tube End
Large fractions of sound waves reflect back and forth in a tube. Different tube lengths cause different resonant frequencies. Small amount of sound waves come out from the tube end or the bell of the
brass instrument. Sound waves reflect at not only closed, but also open ends of tubes.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 23
Signal Reflection in an Open Cable
Cables are usually terminated at the end to eliminate signal reflection. An open cable causes a reflected waveform with same polarity as the transition signal.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 24
An Application: CAKE Clocking
When a signal is sent through a cable, the cable lengths can be different and may change with temperature.
When the pulse is allowed to reflect back, a cake shaped signal is seen at the transmitting end. The width of the cake base can be used to monitor cable lengths.
V/4
R
TDC
w V/4
R
TDC
dA
dB
wdA
dB
w+2dA
w+2dB
w
1
23
1+3
1
2
3
1+3
1 2
3
1 2
3
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 25
Oscilloscope View of the CAKE
Two cables with different lengths are used.
CH1 & 3: Transmitting ends.
CH2 & 4: Receiving ends.
Cake shaped pulses are seen at the transmitting ends.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 26
Why a medium has two independent wave properties? A medium has two independent wave
properties: Speed of wave, or index of refraction Impedance
An oscillation is a process of energy exchange between two energy formats: Kinetic energy and potential energy Electrical energy and magnetic energy
The responses of a media to the two energy formats produce two independent wave properties.
Z
v 1
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 28
Shock Wave of Supersonic Objects
When an object is faster than the speed of sound in air, a shock wave is generated. Bursting balloon: sonic boom. Sneezing: 31 m/s. Initial speed could be higher.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 29
Visible Shock Waves
Supersonic objects cause shock waves. Shock waves cause the water vapor to condense into small ice crystals.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 30
Wake Waves of High Speed Boats
When the speed of a boat is faster than the speed of water wave, a strong wake wave is generated.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 31
Cherenkov Radiation Generated by Fast Charge Particle
When a charged particle moves faster than speed of light in a medium, Cherenkov light is generated.
Faster than speed of light? It is OK in a medium: Speed of light in water: (1/n)*c = (1/1.33)*c
= 0.75 c. Electron at 10 MeV: 0.998 c. Proton at 5 GeV: 0.98 c.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 32
Cherenkov Counter Using Gas
When a particle with speed higher than (1/n)*c passes through the gas, Cherenkov light is generated. Curved mirror focus the light to the photo-multiplier tube (PMT) array. Particle species can be identified. The index of refraction n is adjusted by changing the pressure of gas.
pion
proton
PMTArray
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 33
Observation of Cherenkov Light in Atmosphere
Cherenkov light can be generated in atmosphere when cosmic ray particles pass through.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 34
Cherenkov Light in Liquid
Super-Kamiokande water Cherenkov detector
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 35
Cherenkov Light in Solid
The detector is used to detect high energy protons for LHC experiments at CERN.
Cherenkov light is generated in fused quartz. Generated light is under total reflection inside the L-shaped bar. (Therefore
the index of fraction of the medium must be > 1.414. ) The light reach the silicon photo multiplier (SiPM) and a electrical pulse is
generated.
SiPM
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 37
Waves in Media
Two lights (ordinary and extraordinary) in a crystal have different speed and polarizations. Two acoustic waves can be generated in an isotropic solid. Three acoustic waves can be generated in a crystal.
EM WavesOptics
Mechanical WavesAcoustics
Fluid(Gas, Liquid)
1 transverse wave 1 compression wave
Isotropic Solid(Glass, Fused Quartz)
1 transverse wave 2 waves (P and S)
Anisotropic Solid(Crystal)
2 waves (o and e) 3 waves (P, S and S’)
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 38
Lights in a Calcite Crystal
Lights with different polarizations have different speed in a Calcite crystal. The phenomenon is called birefringence (double refraction).
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 39
Earthquake
The P wave generated by an earthquake arrives earlier than S wave in a seismogram. The distance of the earthquake focus can be estimated from the arrival time difference of the P and
S waves.
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Color on Plastic CD Box
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 40
sky
It is not due to interference on thin film.
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Birefringence (Double Refraction) Due to Internal Stress (Photoelasticity)
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 41
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The Residual Stress in Plastic Film
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 43
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Polarization of Reflection
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 45
Brewster Angle
tan(B ) n2
n1
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Colors Due to Multiple Effects
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 46
sky
Polarized lights are generated in the sky due to scattering. Residual stress in plastic causes double refraction. Double refraction causes polarization plane to rotate and the amount of
rotation is a function of the wavelength. Reflectivity of the plastic surface depends on the direction of the
polarization.
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Complexity (or Fun) of Wave Physics
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 47
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 48
Complexity of Wave Physics
Solid media cause more waves interacting each other. Speeds of waves may depend on the wavelength, i.e., dispersive. Large amplitudes cause the wave equations become non-linear or even chaotic.
Linear range Non-linear range Chaos
Non-dispersive
Dispersive Non-dispersive
Dispersive
Fluid
Isotropic Solid
Anisotropic Solid
College Optics
Earthquake
Tsunami
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 49
Nonlinear Optics
There are many amazing effects in nonlinear domain. Frequency of waves can be doubled in nonlinear crystals. When a 1064 nm (infrared) laser is sent through a nonlinear optical crystal
(KDP), a 532 nm light (green) can be generated.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 50
Geological Strata
The earthquake waves travel in layered solid media. The media are usually simplified as isotropic.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 51
Anisotropic Geological Strata?
In reality, rocks can be anisotropic. How rocks become anisotropic is not well understood.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 52
Tsunami
An earthquake sends waves from layers solid to water in deep ocean to start a tsunami. Near the sea shore, the tsunami becomes a shallow water wave which is both dispersive and
nonlinear (or chaotic).
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Finale: Why Sine Function is Special
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 53
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 54
Demo: Reproducing Voice with a Piano
All students come to stage. Howl a vowel into the piano.
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Fourier Analysis
Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 55
x(t) a0 a1 sin(t 1) a2 sin(2t 2) a3 sin(3t 3) ...
Periodic oscillations are decomposed into different frequency components.
Corresponding piano strings resonate.
External oscillation stops, but vibration of piano strings continues.
Human voice is thus synthesized.
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 56
Fourier Series
Any periodic function can be expanded into a Fourier series. Mathematically, a periodic function can also be expanded into
other series. Why do we choose the Fourier series?
x(t) a0 a1 sin(t 1) a2 sin(2t 2) a3 sin(3t 3) ...
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 57
Taylor Expansion
Using Taylor expansion, a function can be decomposed into linear term and non-linear terms.
Is this decomposition artificial?
f kx bx 2 cx 3 dx 4 ...
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Aug. 2013, Wu Jinyuan, Fermilab [email protected] Wave Phenomena 58
Coexistence of Fourier series and the Taylor expansion
The Fourier series is not merely a mathematic expression. There exist physical systems oscillating this way.
x(t) a0 a1 sin(t 1) a2 sin(2t 2) a3 sin(3t 3) ...
f kx md2xdt 2 kx 0 x(t) A1 cos(t) B1 sin(t)
f kx bx 2 cx 3 dx 4 ... The recovery force of real system may not be linear. But it can be arbitrarily close to linear when the amplitude is
arbitrarily small. Linear recovery force causes simple harmonic oscillation:
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The End
Thanks