Phase change from mass in middle of a string

In summary, the reflection coefficient r can be expressed as r = e^(iφ) and the phase change φ can be expressed as φ = Im(ln(-ip/(1+ip))). This equation accounts for the expected behavior of the phase change for both small and large values of p, corresponding to small and large masses M, respectively.
  • #1
Koranzite
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Homework Statement



There is a mass M in the middle of an infinite string, of the same linear density on both sides. The reflection coefficient is [itex] r=-ip/(1+ip) [/itex] where [itex] p=ω^2 M/2Tk [/itex]
How does the phase change on reflection vary with M, for fixed ω and T?

Homework Equations



Phase change = Im(r)/Re(r)

The Attempt at a Solution



I got the expression [itex] \varphi =arctan(1/p) [/itex], which I can't see how it could be right, as it implies that a phase change of [itex] \pi/2 [/itex] occurs when the mass is 0. I know that when the mass is 0, there should be no phase change, and it should tend to [itex] \pi [/itex] as the mass tends to infinity (but the arctan function has a maximum value of [itex] \pi/2 [/itex]). How can I resolve this to get an equation for the phase change that works?
 
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  • #2


Hello,

Your attempt at a solution is on the right track, but you are correct in noting that it does not account for the expected behavior when the mass is 0 or infinity. This is because the arctan function has a limited range of values, as you mentioned.

To resolve this, we can use the fact that the reflection coefficient r can also be written as r = e^(iφ), where φ is the phase change. This means that we can express the phase change as:

φ = Im(ln(r)) = Im(ln(-ip/(1+ip))) = arctan(p)

This expression gives us the correct behavior for both small and large values of p. When p is small (corresponding to a small mass M), the phase change is close to 0, which is what we expect since there should be little to no phase change when there is little mass present. When p is large (corresponding to a large mass M), the phase change tends to π, which is what we expect since a large mass should result in a significant phase change.

I hope this helps clarify the issue. Good luck with your research!
 

FAQ: Phase change from mass in middle of a string

What is "Phase change from mass in middle of a string"?

Phase change from mass in middle of a string refers to the phenomenon where a mass is added to the middle of a string, causing a change in the phase of the string's vibration.

How does the addition of a mass in the middle of a string affect its vibration?

The addition of a mass in the middle of a string changes the frequency and wavelength of the string's vibration, resulting in a different phase or pattern of vibration.

What factors determine the phase change in a string when a mass is added to its middle?

The factors that determine the phase change in a string include the mass of the added object, the tension of the string, and the length of the string.

Can the phase change in a string be predicted or controlled?

Yes, using mathematical equations and principles such as the wave equation and the principle of superposition, the phase change in a string can be predicted and controlled to a certain extent.

What are some real-world applications of phase change in strings with added masses?

Phase change in strings with added masses has various applications, including musical instruments such as guitars and pianos, acoustic imaging techniques, and seismic monitoring in geology.

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