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March 17 |
March 18 |
March 19 |
March 20 |
March 21 |
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we'll do in class |
lab E1 you must bring a calculator on which you know how to find the standard deviation! |
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(always done before class) |
& doppler shift (there are 2 mistakes in the doppler shift section.... one, everyone should notice; the other, probably only the astro people will notice) what could be better than class and a movie? |
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| in-class
presentation |
spend
20 minutes trying to find the L square matrix and the v column matrix
such that 1) v' = L v 2) v =(something times x something times ct) 3) the L matrix is such that LT = L-1 |
what
are the two mistakes that the book makes in the doppler shift section? |
questions
I expect you to think about and have answers: a) what L is equivalent to L-1 ? i.e., L(?) = L-1(v/c) b) is L(u/c) L(v/c) = L(v/c) L(u/c) ?? i.e., is L commutative in 1 dimension? in 3 dimensions? c) let's define L(u/c) L(v/c) = L(w/c) what is w/c in terms of u/c and v/c? d) can we apply the Doppler shift formula to the heartbeat problem that we did earlier (1-12)? |
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homework (by 5 pm) |
because there will be homework on thursday |
1(28,
14) please do 28 as a length contraction problem |
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1) one time dilation 2) one doppler shift CORRECTION! since we didnt get to watch teh whole movie tuesday, I will let you turn in question 1 only if you want, and delay (sadly) question 2 till after miniterm/spring break (but will anybody remember how to do it then??) should you choose |
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if you are missing class thursday, you can start any time!! |
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Particle Physics booklet here |
doppler effect applet |
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March 10 |
March 11 |
March 12 |
March 13 |
March 14 |
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we'll do in class |
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(always done before class) |
or how perpendicular lengths got into the absolute column length contraction: pp. 18-20 (this was supposed to be for yesterday) |
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although i see that you were actually supposed to do that for last monday! |
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| in-class
presentation |
you
will have found equations for x-bar and y-bar in terms of x, y,
and theta also, you will have calculated "the interval" for the two events (1. muon is created & 2. muon reaches ground) let's re-define "the interval" as Dx2 - c2Dt2 so that it isn't imaginary; if you already used the other one |
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homework (by 5 pm) |
& remember: no numbers until the absolute last line of the problem |
now Tonya stands at the back of the train, where the light also is... consider the two events" 1) light leaves the back of the train 2) light returns to the back of the train Since you know the time between the two events according to Tonya, you can do a time dilation problem to find the time interval according to Reid; but Reid can also solve the problem by doing a d-v-a-t, even though he doesnt initially know the length of the train, according to him. By equating the two method's answers, show that the train length according to Reid is g (gamma) times smaller than the length of train according to Tonya see the applet light_beam_clock.htm at T:\Student\kolena\Relativity_Physlets\ contents\s_relativity\sp_rel\ use the bottom light beam clock |
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.... and remember to solve for v/c, NOT v |
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order your Particle Physics booklet here order the 320-page 2006 edition |
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March 3 |
March 4 |
March 5 |
March 6 |
March 7 |
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and course expectations look at the textbook Table of Contents |
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bring a copy
of "The Complete Guide to Force Diagram Solutions" to class (and have read it?) |
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make sure you have your calculator
for class today (I don't want to send you back) |
| what
we'll do in class |
what IS modern physics anyway?? |
how do we make N's 1st law still true, even though there appear to be violations |
finish centrifugal/coriolis force exploration |
begin classifying physics quantities (simultaneity, position, velocity, time intervals, etc.) as to whether they are relative or absolute to different observers your book does one of these in the section 1(5) reading for today |
learn the "time dilation" problem-solving procedure talk about g apply to problem 1(10) |
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(always done before class) |
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think one example of each type of violation of N's 1st law: an object that has a = 0, yet feels a net force an object that has no net force on it, yet is accelerating in each case, you must specify the reference frame, and also the object you are talking about (please dont repeat generically the examples we have had so far!!) |
green handout: "Rotataing Frames of Reference; Inertial Forces" |
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finish section 1(5), i.e., pp. 16-17 |
| in-class
presentation |
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homework (by 5 pm) |
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(remember that there are see the applet Rel_of_Simultaneity.htm at T:\Student\kolena\Relativity_Physlets\ contents\s_relativity\sp_rel\ |
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thrown south from the pitcher's mound to home plate, at a reasonable speed, in Durham (or the displacement of any sports ball, kicked, thrown, or hit) document the numbers you assume to start the problem |
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