Calculating Next 3 Harmonics of a Standing Wave

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To calculate the next three harmonics of a standing wave given the first harmonic with length L, the wavelengths are derived from the relationship that nodes are located at fixed endpoints. The first harmonic has a wavelength of (4/3)L, while the second harmonic's wavelength is (2/3)L. The frequency can be calculated using the formula velocity = wavelength * frequency, maintaining the same wave speed for all harmonics. Standing waves with one fixed and one open end only support odd-numbered harmonics due to the boundary conditions, which restrict the formation of even harmonics. Understanding these principles allows for the determination of frequencies and wavelengths for the subsequent harmonics.
Nano
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Homework Statement


Given the first harmonic, with length L, of a certain standing wave, what is the process for coming up with the next 3 harmonics for it?

Homework Equations


velocity = wavelength * frequency

The Attempt at a Solution


I don't understand how to draw the "next harmonic". I've come up with a formula for wavlenth of the first harmonic:
= (4/3)L
and with that, frequency
= (3v)/(4L)
 
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Take a butchers at this...

http://id.mind.net/~zona/mstm/physics/waves/standingWaves/standingWaves1/StandingWaves1.html"
 
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Nano said:

Homework Statement


Given the first harmonic, with length L, of a certain standing wave, what is the process for coming up with the next 3 harmonics for it?


Homework Equations


velocity = wavelength * frequency


The Attempt at a Solution


I don't understand how to draw the "next harmonic". I've come up with a formula for wavlenth of the first harmonic:
= (4/3)L
and with that, frequency
= (3v)/(4L)

Well, for a standing wave the ends are fixed and therefore are nodes. In a sinusoidal wave the nodes are half a wavelength apart. In a string of length L, standing vibrations may be set up by different frequencies that give rise to waves that will have nodes at the endpoints. These wave will have wavelengths,

\lambda = 2L, \frac{2L}{2}, \frac{2L}{3},..., \frac{2l}{n}

The wave speed c is the same for all frequencies, and as you say, c = f \lambda

This should be enough for you to deduce the frequencies and the wavelengths of the harmonics (or overtones as they are sometimes called).
 
So as I've said that the wavelength of the first harmonic =(4/3)L, that means the wavelength of the second harmonic
= (4/3)L / n = (4/3)L / 2 = (2/3) L

Is this right?

By the way, the wave has a node at one end and is open at the other. In class we learned that standing waves with one open/one fixed end have only odd numbered harmonics. Why is this?
 
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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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