Wave Pulse - Finding Average Transverse Acceleration of Segment

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A traveling wave pulse moves at 6 m/s across a string, with a segment showing an angle change from 17 degrees to zero over a distance of 3 mm. The discussion focuses on calculating the average transverse acceleration using the wave equation and the relationship between velocity and angle. The user initially attempts to derive acceleration from the second derivative of position but struggles with the concavity term. They then apply their intuition to relate average transverse acceleration to the slope of the wave at a specific point, ultimately realizing that approximating derivatives as a power series is necessary for the solution. The problem specifically asks for the average transverse acceleration of the string segment.
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Homework Statement


A traveling wave pulse is shown in figure 1 below, traveling at v=6 m/s across a string. In figure 2, a short segment of the string is shown zoomed in. The angle of this string goes from θ1 = 17o to zero within a small horizontal distance Δx = 3 mm.

wave%20concavity.jpg


Homework Equations


∂^2y/∂x^2= 1/v2 * (∂^2y/∂t2^2)



The Attempt at a Solution


I know using that equation I want to solve for the acceleration, which is the second derivative of position (y), so I should solve for (∂^2y/∂t2^2) in terms of v, but when I do that I am still left with an equation in terms of ∂^2y/∂x^2, the concavity, which I am not sure what do do with / what it equals.

So next I tried using my intuition:

|average transverse acceleration| = |Δv|/Δt = initial transverse velocity / Δt.

And since initial transverse velocity = the slope of the graph at point 1 (where Δx begins) = rise/run = tan(θ), and Δt = Δx/v, the above eqn becomes:

( v * tan(θ) ) / Δx

But that isn't right
 
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I believe you are supposed to approximate ##y(x, t) ## and ## \frac {\partial^2 y} {\partial x^2} ## as a power series in the vicinity the crest and then use the given values to estimate whatever coefficients you will end up with.
 
You know that dy/dx varies from 0 to tan(17) over a distance Δx=3 mm.
You can approximate the derivative of f(x)=dy/dx as Δf/Δx. And this will be the left term of your equation.
 
Thanks guys! Approximating the derivative of f(x)=dy/dx as Δf/Δx did the trick.

Also, for reference purposes if anyone is reading this thread in search of an answer to a similar problem, I forgot to explicitly mention in my OP that the problem question states: "What is the (average) transverse acceleration of this string segment?"
 
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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