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Music, Math, and Motion with Dr. Arun Chandra & Dr. E.J. Zita The Evergreen St. College Fall week 3 Tuesday 14 Oct. 2008.

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Presentation on theme: "Music, Math, and Motion with Dr. Arun Chandra & Dr. E.J. Zita The Evergreen St. College Fall week 3 Tuesday 14 Oct. 2008."— Presentation transcript:

1 Music, Math, and Motion with Dr. Arun Chandra & Dr. E.J. Zita The Evergreen St. College Fall week 3 Tuesday 14 Oct. 2008

2 Overview Syllabus for the next two weeks Contact: –Radio waves –21 cm line and its frequency –Estimate the chance of extraterrestrial intelligence Loy Ch.8: –Easier way to derive frequencies –Springs, strings, and pipes –Resonant wavelengths and Q factor

3 Syllabus for the next two weeks

4 Contact –Radio waves –21 cm line and its frequency –Estimate the chance of extraterrestrial intelligence

5 Radio waves and EM spectrum

6 21-cm line of Hydrogen http://abyss.uoregon.edu/~js/ast122/lectures/lec22.html

7 21 cm line and its frequency What would be the frequency of radio waves of wavelength = 21 cm?

8 Circular polarization http://www.nsm.buffalo.edu/~jochena/images/circular3.gif

9 Estimate possibility of ETI

10

11 http://www.activemind.com/Mysterious/Topics/SETI/drake_equation.html

12 Loy Ch.8: Vibrating Systems –Easier way to derive frequencies –Springs, strings, and pipes –Resonant wavelengths and Q factor

13 Simple Harmonic Motion (SHM) Loy p.130 s

14 Kinematics of oscillations

15 Easier way to derive frequencies Compare to p.241-241 in Loy (harder, but same result) for SPRING OSCILLATION:

16 Easier way to derive frequencies F = ma -k x = m  2 x k = m  2  2 = k/m  =  k/m = 2  f

17 Frequency of air in piston What instruments are like this? What is the spring constant k of air? Recall that F = -kx, so the units of k are those of F/x, or (N/m). Recall that Pressure = Force/Area, so P = F/A or F = PA. For air, where  = a constant and l = the length of the chamber in which air is trapped.

18 Springs, strings, and pipes Nodes = still points at equilibrium Antinodes = points of maximum oscillation

19 Springs, strings, and pipes How many waves fit in the length L? Use that to find the resonant wavelengths n and resonant frequencies f n.

20 Springs, strings, and pipes How many waves fit in the length L? Use that to find the resonant wavelengths n and resonant frequencies f n.

21 Conical pipes Displacement must vanish at opening, therefore

22 Resonance: Q factor Sharpness of resonance

23 Galloping Gertie http://www.youtube.com/watch?v=j-zczJXSxnw


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