Wednesday, July 19, 2006
Announcements:
- Exam 2 will be held next Monday, which is the same
day as the Lab Exam for many of you. If you prefer to take the
Lab
Exam this Friday instead of on Monday, let me know so that I can make
the necessary arrangements.
- A student in this class (Zach Swan) has identified a website that has
several useful Java Applets
for selected physics topics. I have added a link to this website
under
the Resources section of the course webpage, and I encourage you to
take a look at these as you prepare for your exams.
- Several groups have already published their Web Project.
Please check the list of Web
Projects and let me know of any updates.
- A solution to the Contact Lenses
real-world problem has been posted. Be sure to examine this
solution before the next exam.
Assignments:
- Read Chapter 31 and submit HW31a before class tomorrow.
- HW29b is due tonight at midnight
- Web Projects are due this Friday, July 21. Send me your URL
as soon as possible.
Chapter 29: Relativity
Special relativity deals with
inertial frames of reference (a = 0)
General relativity (a <>
0)
Examples of inertial and non-inertial reference
frames: a) space ship traveling in a straight line, b) space
shuttle in orbit, c) this classroom
Consequences of Special Relativity: As v -> c, several
physical parameters change by factor of gamma = 1/sqrt(1-v^2/c^2)
Ponderable:
What are "relativistic" speeds? (see table below)
Time dilation: t =
to*gamma
Length contraction: L =
Lo/gamma
Mass increase: m =
mo*gamma
Relativistic energy: E =
mc^2 = gamma*Eo
Relativistic KE: K =
Eo*gamma - Eo
General relativity:
All physical experiments yield identical results in
an accelerated reference frame as they do in a gravitational field.
Black holes: Light cannot
escape a star with a radius less than or equal to the Schwarzschild radius: R =
2GM/c^2
Ponderable: If an astronaut travels 1 ly at 0.9c, why is t
<> to*gamma?
Concept
Tests - Chapter 26
Chapter 30: Quantum Physics
"The universe is not only
stranger than we imagine, it is stranger than we can imagine."
This chapter synthesizes many concepts from previous chapters.
Movie trailer from Down the Rabbit
Hole: The
Double Slit Experiment
30-1: Blackbody Radiation and
Quantization
An ideal blackbody
does not reflect any light that hits it. Such a perfect absorber
of radiant energy is also a perfect emitter (e = 1.00).
The distribution of energy as a function of
frequency only depends on the temperature of the blackbody:
Wien's
displacement law: f(peak) = wT, where w = 5.88x1010
s-1K-1
Quantization of energy
Examples of quantization
30-2: Photons and the
Photoelectric Effect
Planck's constant and quantization: En = nhf
Photons and photoelectric effect - energy, work function, cutoff
frequency, max K
KEmax = E - Wo
30-3: Relativistic mass and
momentum of photons
Demo: Radiometer
30-4: Photon scattering and
Compton effect
The de Broglie wavelength, wave-particle duality
Wavelength and resolution
X-ray diffraction
30-5: Heisenberg uncertainty
principle
30-6: Quantum Tunneling
Scanning Tunneling Microscope (STM)
Concept
Tests - Chapter 27