Topics In Astronomy
GES 639
Fall 2007
This is a course intended to enrich your
knowledge of, and tools to use, in Astronomy. The target student is a
present
or future teacher of Earth Science, Physics, or something else.
"Something else" is truly undefined. One legendary Astronomy teacher in
WNY was primarily an English teacher.
The "Topics" designation allows a desirable flexibility, so we
agreed
on part of the Syllabus at our first meeting. This means that you are
reading a second draft of the Syllabus. These topics agreed
upon will take about half the semester. The rest of the Syllabus will
be on the topics of The Astronomy
Teacher's Toolkit, Bad Astronomy, and The Sun.
Texts: "Astronomy For Dummies" (Maran, recommended) Well structured and
indexed, straightforward and correct explanations.
"Bad Astronomy" (Plait, required) An insightful and thorough
introduction to (and answers to) alien beliefs among us.
"The Sun, A Biography" (Whitehouse, required) Not a textbook, not a
biography either. A great read, historical and scientific.
Grades will be based on two exams, assignments, and a presentation.
Aug. 27 A.
Discussion and choice of class-chosen topics
B. Toolkit#1 Planetarium
Experience
1. The planetarium
experience in the seats
2. Discussion of a
planetarium experience in the
"loamlight" (You as the presenter, or at least structuring the
presentation)<>
3. Assignment: Outline of an
original program, due Sept.17, ready to share, 1/2 page max. (We will
not be creating a planetarium program!)
Sept.10: Class Choice Topic#1: Special
Relativity
1. It is a testable theory about
how the express physical laws in moving coordinate systems.
2. Galilean relativity: If an observation is made in
a lab moving with velocity v, a velocity v1 in the lab will move at
v+v1 in the original reference frame. Accelerations will be equal in
both frames. The laws of physics should be the same in both. Common
sense
rules.
3. The laws of electromagnetic theory, Maxwell's
equations, pose a dilemma. The speed of radiation is a calculated constant,
independent of the lab velocity!
4. In 1905, Einstein published a very different
relativity than Galileo's. The need was to be able to calculate the
value of c in any frame, moving or not. It certainly was not consistent
with common sense.
5. Speeds: In a lab of speed v, a velocity v1
would be (v+v1)/(1 + vv1/c2)
6. Accelerations: Accelerations are lower in the
moving system. The speed of light can not be reached by acceleration at
all!
7. Maxwell's equations are the same in the moving
system, as was required.
8. Other observations, e.g. of distance, inertial
mass, time intervals, are different in the moving system. Lorentz
factor = 1/(1- v2/c2)1/2 affects these
properties.
9. Tests: Constancy of c in moving system. Lifetime
of muons at reletivistic speeds. Thickness of atmosphere to a cosmic
muon. Acceleration of particles in clyclotrons.
Necessity of synchrotrons.
10. The Doppler effect is a consequence of relativity.
Wavelength of EM radiation depends on the velocity of the emitter:
wavelength/(rest wavelength) = ((1+v/c)/(1-v/c))1/2,
where positive velocity means velocity away from the observer.
The astronomical redshift z = (wavelength - rest
wavelength)/(rest wavelength), = the above
expression - 1.
11. Low velocity limit: For v << c, wavelength
= (rest wavelength) x (1+v/c). (Same sign convention)
12. Mass-energy equivalence: The total energy of an object
depends on the classical energy (chemical + gravitational + kinetic) = EClassical,
but is greater. It can be written as E = (E2Classical
+ m2c4)1/2 (m = classical mass),
or E = mc2 (m is the relativistic mass). At low v, E= EClassical
+ mc2, (m is classical).
13. Tests: Nuclear fission, binding energy of nucleii appears as mass
deficit, annhilation energy, inertial mass depends on velocity (see
above). Neutron decay. Cosmic air showers.
14. Twin paradox discussion.