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?