Dispersion relation for a surface wave of a pool of water

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Homework Help Overview

The discussion revolves around the dispersion relation for surface waves in a pool of water, specifically analyzing the relationship between angular frequency (ω) and wave number (k). Participants explore the mathematical expressions involved, including the role of the hyperbolic tangent function (tanh) and gravitational acceleration (g).

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants attempt to calculate ω for various values of k and question the accuracy of their results. There is discussion about the implications of missing factors in the equations and the behavior of tanh(k) for large and small k. Some participants suggest examining the functional behavior of the equations rather than relying solely on numerical values.

Discussion Status

The discussion is active, with participants providing hints and exploring different interpretations of the problem. Some guidance has been offered regarding the behavior of the functions involved, and there is an ongoing examination of how to approach the graphing of the relationship without direct plotting.

Contextual Notes

Participants note the lack of labeled units on the axes of the graph, which complicates their calculations. There is also mention of specific values for g and the implications of approximations for small and large k in the context of the problem.

Pushoam
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Homework Statement


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Homework Equations

The Attempt at a Solution



## v = \frac { \omega } k ##

## \omega = \sqrt{ kg \tanh (k) } ##I have no idea to guess the graph.

I put g = 9.8 and tried to calculate ## \omega ## for different values of k.

## \omega (0 ) = 0,

\omega (30) = 17.15

~~\omega (20) = 14 ##

But, these values don’t match any of the graph.

So, what to do now?
 

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You missed a factor of ## h ## in ## \tanh (kh) ##. (Editing: Oh I missed the part ## h=1##). One problem with trying to rely on numbers on the axes here is they don't label their units, so you don't know what number to use for ## g ##. ## \\ ## A hint that should help: What is the functional behavior of ## \tanh(k) ## for large ## k ##? Thereby, what does ## \omega ## vs. ## k ## look like for large ## k ##? ## \\ ## Also, what is the slope for very small ## k ##? Is it some constant or is it zero? (Hint: Expand ## \sinh(x) ## and ## \cosh(x) ## in Taylor series for small ##x ##). ## \\ ## You could also try using ## g=980 ## cm/sec^2 , but for this problem, I think that leads you to an incorrect answer.
 
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Charles Link said:
You missed a factor of ## h ## in ## \tanh (kh) ##. (Editing: Oh I missed the part ## h=1##). One problem with trying to rely on numbers on the axes here is they don't label their units, so you don't know what number to use for ## g ##. ## \\ ## A hint that should help: What is the functional behavior of ## \tanh(k) ## for large ## k ##? Thereby, what does ## \omega ## vs. ## k ## look like for large ## k ##? ## \\ ## Also, what is the slope for very small ## k ##? Is it some constant or is it zero? (Hint: Expand ## \sinh(x) ## and ## \cosh(x) ## in Taylor series for small ##x ##). ## \\ ## You could also try using ## g=980 ## cm/sec^2 , but for this problem, I think that leads you to an incorrect answer.
I didn’t know the graph of ## \tanh ( k ) ## and I don’t want to look for it right now. 1st I want to solve this question with the knowledge I have and then I will look to the graph.

## \tanh ( k) = \frac { e^k - e^{-k} } { e^k + e^{-k} } ## ...(.1)

As k tends to infinity, ## \tanh ( k) ## tends to 1.

So, for very large k, ## \omega \approx \sqrt{ kg} ## ...(2)

So, as k goes to infinity, ##\omega## should go to infinity . ...(3)

(b) and (d) fulfils condition (3).## \tanh ( k ) = k \frac { 1 + \frac { k^2}{3!} +…}{ 1 + \frac { k^2}{2!} + …} ## ...(4)

So, for small k, ## \tanh ( k) \approx k ## ...(5)

## \omega \approx k\sqrt{ g} ## ...(6)

So, ##\omega## goes from ##\sqrt{ g}## k for small k to ##\sqrt {gk} ## for large k. This is shown by (b).

So, the correct option is (b).

Is this correct?
 
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Correct=I would pick (b) also. A couple of things to observe: For large ## k ##, ## \omega=\sqrt{g} \sqrt{k} ## so instead of looking like a straight line, the second derivative will be negative. ## \\ ## Also for small ## k ##, ## d \omega /dk=\sqrt{g} ##, rather than 0. ## \\ ## (d) comes close to working in some ways, but the second derivative in (d) is slightly positive for large ## k ##.
 
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Thanks.
Is there any insight article in PF, which helps in understanding how to guess a graph without plotting it exactly?
 
Pushoam said:
Thanks.
Is there any insight article in PF, which helps in understanding how to guess a graph without plotting it exactly?
Not that I know of. I thought of one additional feature though that helps to show (b) is correct: For large ## k ## (in this case even 18 is large), ## \omega(36)/\omega(18) ## needs to be approximately ## \sqrt{36/18}=\sqrt{2} ##. This would rule out (c).
 
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Charles Link said:
Not that I know of. I thought of one additional feature though that helps to show (b) is correct: For large ## k ## (in this case even 18 is large), ## \omega(36)/\omega(18) ## needs to be approximately ## \sqrt{36/18}=\sqrt{2} ##. This would rule out (c).
That's a nice idea to get rid of g.
Then I can have one ratio for small k and another ratio for large k and see which graph meets this ratio. If I got one meeting this ratio, then surely this will be the required graph.
I see that tanh (k) ≈ k is a good approximation for k < 0.5,
tanh (k) ≈ 1 is a good approximation for k > 10.

Now, small k approximation is not useful here due to scale of the graphs. So, one can use large k approximation to eliminate some options.
Thanks for it.
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