Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

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Chapter 40 Serway & Jewett 6 th Ed.
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Transcript of Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Page 1: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Chapter 40Serway & Jewett 6th Ed.

Page 2: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.
Page 3: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Approximate Total Absorption Cavity

Page 4: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.
Page 5: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

I = T4 = 5.6699 10-8 W/m2-K4

Stefan- Boltzman Law

Page 6: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Ultraviolet Catastrophe

4

2

Tck

I B

Classical expressionClassical expression

Page 7: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Quantized Energy Levelsof a Harmonic Oscillator

Page 8: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Fig 40-9, p.1292

Photoelectric EffectPhotoelectric Effect

Page 9: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Photoelectric EffectPhotoelectric Effect

Page 10: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Table 40-1, p.1294

Page 11: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Electrons interacting with lightClassical Picture

Electrons interacting with lightClassical Picture

kqvBBvqF ˆ

kqvBBvqF ˆ

Just dipole radiation independent of !

Just dipole radiation independent of !

Page 12: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.
Page 13: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Compton ScatteringCompton Scattering

Electrons interacting with lightQuantum Picture

Electrons interacting with lightQuantum Picture

cos1' cm

h

eo

cos1' cm

h

eo

Page 14: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

HydrogenHydrogen

Atomic SpectraAtomic Spectra

NitrogenNitrogen

Page 15: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Balmer’s RealizationBalmer’s Realization

Page 16: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.
Page 18: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

k1 – k2 = k

1 – 2 =

k1 + k2 = k

1 + 2 =

Page 19: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

i

ii twA cos

Wavepacket

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Depending on how we do the experiment we determine what happens!

Depending on how we do the experiment we determine what happens!

Delayed Choice

Page 21: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Superposition StatesSuperposition States

01 21 cc 01 21 cc

MeasurementMeasurement

+

or

=

One and only one of One and only one of

=

Page 22: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Photons are emitted on opposite sides of the pump beam, along two cones. One of cone has horizontal polarization and the other of has vertical polarization. Photon pairs emitted along the intersections of the cones are entangled in polarization -- each photon is individually unpolarized, and yet the photons necessarily have perpendicular polarizations, no matter how far apart they are!

Photons are emitted on opposite sides of the pump beam, along two cones. One of cone has horizontal polarization and the other of has vertical polarization. Photon pairs emitted along the intersections of the cones are entangled in polarization -- each photon is individually unpolarized, and yet the photons necessarily have perpendicular polarizations, no matter how far apart they are!

http://www.physics.uiuc.edu/People/Faculty/profiles/Kwiat/index.htmlhttp://www.physics.uiuc.edu/People/Faculty/profiles/Kwiat/index.html

Page 23: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.
Page 24: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

Quantum Weirdness!

Page 25: Chapter 40 Serway & Jewett 6 th Ed.. Approximate Total Absorption Cavity.

What is Schrodinger's Cat Paradox?    Schrodinger's Cat (in his own words)"One can even set up quite ridiculous cases. A cat is penned up in a steel chamber, along with the following diabolical device (which must be secured against direct interference by the cat): in a Geiger counter there is a tiny bit of radioactive substance, so small that perhaps in the course of one hour one of the atoms decays, but also, with equal probability, perhaps none; if it happens, the counter tube discharges and through a relay releases a hammer which shatters a small flask of hydrocyanic acid. If one has left this entire system to itself for an hour, one would say that the cat still lives if meanwhile no atom has decayed. The first atomic decay would have poisoned it. The Psi function for the entire system would express this by having in it the living and the dead cat (pardon the expression) mixed or smeared out in equal parts. It is typical of these cases that an indeterminacy originally restricted to the atomic domain becomes transformed into macroscopic indeterminacy, which can then be resolved by direct observation. That prevents us from so naively accepting as valid a "blurred model" for representing reality. In itself it would not embody anything unclear or contradictory. There is a difference between a shaky or out-of-focus photograph and a snapshot of clouds and fog banks." -- Erwin SchrodingerTranslation by John D. TrimmerBasically what Schrodinger is saying is that because of the way the experiment is set up, the cat has a 50% chance of being alive, and a 50% chance of being dead. It is just as likely that the cat is alive as that it is dead, so Schrodinger said that until the box is opened, the cat is both alive and dead. This is obviously false, the cat cannot be both alive and dead at the same time. This problem is meant to illustrate a theory of quantum mechanics called "indeterminacy." Indeterminacy says that there can be more than one correct answer to a problem which physically can only have one answer. Schrodinger came up with this illustration to demonstrate that there was a problem with this theory of quantum mechanics.