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Cosmology, Astronomy and Modern Physics

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Wave-particle duality. Applying this to the atom: Heisenberg saw a way to resolve the particle and wave concept of an electron ... – PowerPoint PPT presentation

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Title: Cosmology, Astronomy and Modern Physics


1
Quantum Mechanics
2
The New Quantum Era
Erwin Schrödinger 1887-1961
Werner Heisenberg 1901-1976
Paul Dirac 1902-1984
3
Wave-particle duality
  • Applying this to the atom
  • Heisenberg saw a way to resolve the particle and
    wave concept of an electron without using the
    Bohr model

Max Born 1882-1970
Born suggested matrix mechanics
Worked.but no physical picture
Paul Ehrenfest and Pascual Jordan 1880-1933
1902-1980
4
Schrödinger
  • Matter waves? - Schrödinger wave equation
  • Wave function ? describes amplitude of wave
  • wave mechanics

1-dimensional Schrödinger equation
Erwin Schrödinger 1887-1961
Quantum mechanics aims to find ? in a certain
situation (e.g. for an electron in an atom)
5
What does it mean?
  • Whole subject in itself
  • We will look at how ? can be interpreted
  • Amplitude of matter wave?

Max Born 1882-1970
?2 can be interpreted to represent the
probability of finding the electron at a given
position at a certain time
No certainties...
6
Double-slit - revisited
  • One electron at a time seemingly random picture

Am. J. Phys. 57 117 (1989)
7
Double slit -probabilities
  • High peaks represent high ?2 high probability

8
Measurements
  • We know that we cant measure very precisely -
    always errors
  • If you measure the weight of a rock, how accurate
    can you be?
  • If you measure the length of something?

Absolute limit to accuracy Not down to
instruments but to nature.
9
Heisenberg
  • The actual act of measuring leads to an
    uncertainty in the measurement

Werner Heisenberg 1901-1976
Overall, the combined uncertainty is given by
Heisenbergs uncertainty principle
You cant measure both the position and momentum
of an object precisely at the same time.
10
Example
  • Say that we can measure the position of an object
    so that the uncertainty is ?x 1.2 x 10-11m.
    Determine the minimum uncertainty in the momentum
    of the object.

4.4 x 10-24 kg ms-1
Very small uncertainty in momentum! What effect
would this have?
11
Example continued
  • If this was an electron (m9.1 x 10-31 kg), what
    would be the uncertainty in its speed? What if
    it were a baseball (m0.15kg)?

p mv so ?p m?v and thus ?v ?p/m
?v (electron) (4.4 x 10-24) / (9.1 x 10-31)
4.8 x 106 ms-1 ?v (baseball) (4.4 x 10-24) /
(0.15) 2.9 x 10-23 ms-1
So very small uncertainty in velocity of baseball
(negligible) but MASSIVE uncertainty in velocity
of electron. Think of it round the other way - if
you know the velocity...
12
Uncertainty 2
  • Distance is related to time (?t ?x/v)
  • Energy related to the velocity (momentum) hf
    hv/?
  • So another version of the uncertainty principle
    is

This would, in principle, allow us to borrow
large amounts of energy for a very short period
of time
13
Quantum Measurement
  • The very act of measurement affects what youre
    measuring
  • States indeterminate until they are measured
  • collapse of the wavefunction

14
Schrödingers Cat
  • Schrödinger unhappy with the probabilities...
  • ? Famous thought experiment.

15
The cat is dead and alive?
  • Until we open the box and observe, we dont know
    if the decay has happened or not
  • The cat is dead
  • The cat is alive

superposition of states
But once we make the observation open the box
we collapse the wavefunction. Maybe the cat does
this by itself
16
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17
Copenhagen Interpretation
  • In honour of Niels Bohr
  • A collection of ideas
  • Ideas of probability, complementarity and
    self-consistency

Bohr at Los Alamos
18
Dirac
  • Synthesis of relativity and quantum theory
  • Prediction of anti-matter

Paul Dirac 1902-1984
1932 investigation of cosmic rays
Found particle with mass of electron, but
positive charge positron
Carl Anderson 1905-1991
19
Cloud Chamber
  • Gas cooled to condensation point
  • High energy particles leave droplets behind

Charles Wilson 1869-1959
See also bubble chamber
20
Solvay, 1927
Heisenberg
Schrodinger
Pauli
Debye
Bragg
Dirac
Compton
Born
de Broglie
Bohr
Planck
Curie
Lorentz
Einstein
Wilson
21
EPR paradox
  • Einstein, Podolsky and Rosen
  • Separation of two entangled particles

Measuring the properties of one automatically
defines the properties of the other Spooky
action at a distance Non-locality
John Bell 1928-1990
Alain Aspect b. 1947
22
Many Worlds Interpretation
  • collapsing wave function unsatisfactory
  • Hugh Everett, 1957 (PhD thesis)

Hugh Everett III 1930-1982
Cat is dead and alive Different realities
Strange, but it works gt 50 acceptance amongst
physicists (?)
23
The Macroscopic World
  • Cartoon

24
Back to reality
  • We saw earlier that X-rays were of a suitable
    wavelength to be diffracted by crystals (of the
    order of 10-10 m)

Clifford Schull 1915-2001
Neutrons (m1.675 x 10-27 kg) so
Put ?10-10m v 4000 ms-1
25
Nuclear Physics
  • Next Section
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