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Final Exam

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Title: Final Exam


1
Final Exam
  • Comprehensive
  • Date Tuesday May 4, 2004
  • Location MSC 220
  • Time 6-8 pm

2
27.6 Photons and Electromagnetic Waves
  • Light has a dual nature. It exhibits both wave
    and particle characteristics
  • Applies to all electromagnetic radiations
  • The photoelectric effect and Compton scattering
    offer evidence for the particle nature of light
  • When light and matter interact, light behaves as
    if it were composed of particles
  • Interference and diffraction offer evidence of
    the wave nature of light

3
Possible Application of the Particle Feature in
Space
  • Sunlight striking the sail creates a force that
    pushes the spaceship away from the sun, much as
    the wind propels a sail-boat.

4
27.7 Wave Properties of Particles
  • In 1924, Louis de Broglie postulated that because
    photons have wave and particle characteristics,
    perhaps all forms of matter have both properties
  • Furthermore, the frequency and wavelength of
    matter waves can be determined

5
Matter waves The de Broglie Wavelength and
Frequency
  • Since a photon travels with speed of light, we
    treat it as a massless particle with the
    momentum
  • pE/chf/ch/l (Photons only m0!)
  • Wavelength of the matter wave 
  • lh/ph/(mv) (Classical particles m?0!) 
  • A particle has a wave with frequency fE/h
    associated with it!

6
The Davisson-Germer Experiment
  • In 1927, Davisson and Germer, working at Bell
    Labs, were studying the nature of the surface of
    a nickel crystal by directing a beam of electrons
    at the surface and observing the electrons
    reflected at various angles. They found that the
    electrons were reflected in almost the same way
    that x-ray would be reflected. The results gave
    strong support to de Broglies hypothesis.

7
The Transmission Electron Microscope
  • The electron microscope depends on the wave
    characteristics of electrons
  • Microscopes can only resolve details that are
    slightly smaller than the wavelength of the
    radiation used to illuminate the object
  • The electrons can be accelerated to high energies
    and have small wavelengths

8
27.8 The Wave Function
  • In 1926 Schrödinger proposed a wave equation that
    describes the manner in which matter waves change
    in space and time
  • Schrödingers wave equation is a key element in
    quantum mechanics
  • Schrödingers wave equation is generally solved
    for the wave function, ?

9
Wavefunction, cont.
  • In quantum mechanics ???2 is proportional to the
    probability of finding the particle at a given
    location.

The probability of finding the ground state
hydrogen electron (n1) as a function of the
radial distance from the proton.
10
The Wave Function, final
  • The wave function depends on the particles
    position and the time
  • The value of ???2 at some location at a given
    time is proportional to the probability of
    finding the particle at that location at that time

11
27.9 The Uncertainty Principle
Moving car
Past
Future
-x
x
Now
12
The Uncertainty Principle, cont.
  • What means exact? ? Deterministic view of nature
  • ? This is ok in our world! But not in the world
    of the electron

13
The Uncertainty Principle, cont.
  • (a) A photon hits an electron and (b) transfers
    momentum to the electron.

The observation "destroys" the phenomen
14
The Uncertainty Principle, cont.
  • It is impossible to know (or to measure)
    simultaneously an electrons EXACT position and
    momentum!
  • Erwin Schroedinger (1887-1961) and Werner
    Heisenberg (1901-1976) independently developed a
    new branch of physics called quantum mechanics.
    Quantum theory (its a small world!) predicts
    limits on the accuracy of measurements. This idea
    was introduced in 1927 by Heisenberg and
    complemented Schroedingers wave theory.

15
The Uncertainty Principle, cont.
To see more clearly into the nature of
uncertainty, we consider electrons passing
through a slit
Momentum uncertainty in the y component
We apply the formula for single slit diffraction,
sin?l/W, and postulate that l is the de Broglie
wavelength.
16
The Uncertainty Principle, cont.
  • sinq?tanq (for small q)
  • tanqDpy/px ? Dpy/px?l/W

17
The Uncertainty Principle, cont.
  • Since the electron can pass the slit through
    anywhere over the width W, the uncertainty in the
    y position of the electron is DyW.
  • DpyDy?h

18
The Uncertainty Principle, cont.
  • Heisenberg found that at the very best
  • DpyDy?h/(4p)

Momentum
Position
Uncertainty
19
The Uncertainty Principle, cont.
  • Dy/c?l/c ? Dt?l/c (This is the time that the
    particle needs to traverse its own uncertainty,
    which is on the order of its wavelength)  
  • DE?hc/l
  • (DE)(Dt)?(hcl)/(lc)
  • (DE)(Dt)?h

20
The Uncertainty Principle, final
(DE)(Dt)?h/(4p)
Energy uncertainty of a particle when the
particle is in a certain state
Time interval during which the particle is in the
state
21
  • Example Assume the position of an object is
    known so precisely that the uncertainty in the
    position is only Dy1.5?10-11 m. Determine the
    minimum uncertainty in the momentum of the object
    and find the corresponding minimum uncertainty in
    the speed if the object in an electron.
  • Dpyh/(4pDy)(6.63?10-34 Js)/(4p1.5?10-11 m)
  • Dpy3.5?10-24 kgm/s ? small
  • DvyDpy/m(3.5?10-24 kgm/s)/(9.1?10-31 kg)
  • Dvy3.9?106 m/s ? large

22
Scanning Tunneling Microscope (STM)
  • Allows highly detailed images with resolution
    comparable to the size of a single atom
  • A conducting probe with a sharp tip is brought
    near the surface
  • The electrons can tunnel across the barrier of
    empty space

23
Scanning Tunneling Microscope, cont.
  • By applying a voltage between the surface and the
    tip, the electrons can be made to tunnel
    preferentially from surface to tip
  • The tip samples the distribution of electrons
    just above the surface
  • The STM is very sensitive to the distance between
    the surface and the tip
  • Allows measurements of the height of surface
    features within 0.001 nm

24
Limitation of the STM
  • There is a serious limitation to the STM since it
    depends on the conductivity of the surface and
    the tip
  • Most materials are not conductive at their
    surface
  • An atomic force microscope (AFM) has been
    developed that overcomes this limitation
  • It measures the force between the tip and the
    sample surface
  • Has comparable sensitivity
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