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Simple Harmonic Motion “things that go back and forth”

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Presentation on theme: "Simple Harmonic Motion “things that go back and forth”"— Presentation transcript:

1 Simple Harmonic Motion “things that go back and forth”

2 Our “Spring Chicken” follows a specific sequence to make one full oscillation –Down –Return –Up –Return When the chicken goes below “equilibrium,” (- x) that means the Force is pulling up (+F). Then Chicken goes above “equilibrium,” (+x) and Force is now pushing down (-F). The farther away it goes, the spring just pulls harder to bring it back in the same amount of time! The Thing about Springs...

3 SHM Any periodic motion that is the result of: –A restoring Force that is proportional to the –displacement of the object Is called Simple Harmonic Motion It is explained with “Hooke’s Law:” http://www.subrew.com/chris/fiat/26feb03/spring.jpg

4 Pendulum

5 crest trough - wavelength More waves in the same amount of time means higher frequency. As frequency increases, wavelength decreases! Medium oscillates perpendicular to energy’s direction Medium is a material that can vibrate with SHM

6 Longitudinal Waves Compression R a r e f a c t i o n wavelength Medium oscillates parallel to energy’s direction Period is the time for one wave, oscillation, revolution, swing, etc. to occur Units: sec Think =sec/vib Frequency is the number of vibrations that occur in one second Units: vib/sec Also known as : Hz

7 Frequency & period are inverses of each other The speed of a wave remains constant within a uniform “medium.” With a constant speed, frequency & wavelength are inversely related

8 Springs Pendulum Waves

9 Springs Hey, where’d that “2  ” come from?

10 Pendulums One other type of periodic motion is demonstrated by a pendulum

11 Springs & Motion What would happen if the “Spring Chicken” also moved left –to-right?

12 Wave Behavior Incident Wave: – the point when a wave crosses a medium boundary Reflected wave: –is the returning wave

13 Principle of superposotion Two or more waves combine to form a new wave –The result is called interference Destructive interference – Waves of opposite amplitude meet leading to a zero amplitude point before continuing unchanged Node = zero amplitude point constructive interference –Waves of same amplitude meet leading to greater amplitudes before continuing unchanged Antinode = higher amplitude point

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15 Standing Waves in Strings When the whole string vibrates as one, then it can only fit a crest or a trough, not both. When the frequency is twice as much, the string can now fit one full wavelength. The next opportunity for a whole crest to fit is when there are 2 crests & a trough

16 Definitions: –Node: Points of destructive interference No displacement –Antinode: Points of constructive interference Maximum displacement –Fundamental: basic frequency of a material n=1 –Harmonic: multiples of the fundamental (higher octaves) Standing Waves in Strings

17 Frequency Equations Take all of our general equations for wavelength, and substitute in v/f Strings (2 fixed ends) n = 1, 2, 3 …

18 If we translate the compressions & rarefactions to crests & troughs, we see this: At the fundamental wavelength, one quarter of a wave can fit in the tube at a time. By simply hitting one end of a tube, a compression of air travels the length of the tube. Standing Waves in a Tube One End Closed At the end of the tube, no air can vibrate- it must be a node. The following harmonic must be 5/4 of a wave. What is the pattern here? Every harmonic wavelength must end with a node, so the next harmonic must be ¾ of a wave.

19 Standing Waves in a Tube Both Ends Open Air can vibrate at both ends of the tube- not a node at the end That means that the fundamental is one half of a wave Each harmonic must then be a multiple of one-half of a wavelength

20 Frequency Equations Take all of our general equations for wavelength, and substitute in v/f These are your standing wave equations! Really, there are only two equations to remember… Strings (2 fixed ends) Tubes (1 open end) n = 1, 2, 3 … n = 1, 3, 5 … Tubes (2 open ends) n = 1, 2, 3 …


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