How to Calculate Energy Flux in Traveling Waves with Different Densities?

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Homework Help Overview

The problem involves analyzing the behavior of traveling waves at the junction of two threads with different linear densities under tension. The original poster seeks to determine the ratios of amplitudes for reflected and transmitted waves, as well as to show the relationship between energy flow of the input wave and the sum of reflected and transmitted waves.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationships between wave properties such as amplitude, frequency, and density. There are attempts to derive expressions for kinetic energy and mean energy flux for the waves involved. Questions arise regarding the calculation of power per unit length and the conditions under which the energies of the waves relate to each other.

Discussion Status

Some participants have provided guidance on deriving expressions for kinetic energy and average power, while others express uncertainty about the additive nature of the energies of the incoming, reflected, and transmitted waves. Multiple interpretations of the energy relationships are being explored, and some participants have acknowledged reaching a conclusion.

Contextual Notes

There is a mention of specific ratios of linear densities and the need to consider the implications of these ratios on wave behavior. The discussion also reflects a focus on deriving relationships without providing explicit solutions.

diracdelta
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Homework Statement


Two threads, both having linear density μ1 and μ2 are connected and tensed with tension T.
a) If traveling wave enters onto their junction, find ratios of amplitudes of reflected and input wave, transmitted and input wave, for μ21= 0, 1/4, 1, 4 and infinity
b)
Show that energy flow of input wave is equal to sum of reflected and transmitted wave.

The Attempt at a Solution


As for part a, it is easy.
We have three waves;
Ψin = A cos (ωt - kz)
ψTr = T*A cos (wt -k2z)
ψRef = R*A cos (wt + kz)

R= (Z1-Z2)/(Z1+Z2), T= 1+ R
Z=(T0*μ)1/2
-> R=[(T01)1/2-(T02)1/2]/[(T01)1/2+(T02)1/2]=...=[(1-(μ21)1/2]/[(1+(μ21)1/2].
It is trivial to find those values now.

As for part b)
"The mean energy flux is
eimg332.gif
, also written as
eimg333.gif
and called I, the intensity. For a traveling wave,
eimg335.gif
"
quoted from (http://scienceworld.wolfram.com/physics/EnergyFlux.html)
while i assume, U is potential energy.
So basically, I need to find flux for those three waves, and prove statement.
How to find mean of U as for traveling waves?
 
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Not sure of the exact formula, but for this question you only need to understand how the power in a wave depends on amplitude, frequency and density of medium. Consider a small element of length dx. Mass = ##\rho dx##. If its motion is given by ##y = A \sin(\omega t)##, what is its velocity at time t? What is its KE at time t? What is its average KE over time?
Once you have that, figure out the power per unit length in each of the three waves.
 
Velocity is derivative of y in respect to t -> v =dy/dt= wAcos(wt)
Kinetic energy is is 1/2 ρdx (dy/dt), so average is integral of that expression = .. = 1/4 ρ*A2*w2
(we loose cosine because average of cos squared is 1/2)
 
diracdelta said:
Velocity is derivative of y in respect to t -> v =dy/dt= wAcos(wt)
Kinetic energy is is 1/2 ρdx (dy/dt), so average is integral of that expression = .. = 1/4 ρ*A2*w2
(we loose cosine because average of cos squared is 1/2)
Good. Now, in the present case, w is the same for all three waves, so we can leave that out, and the 1/4, and get that it is k ρA2 for some constant k.
Substitute in the values of density and amplitude for each of the three waves. Do the transmitted and reflected power add up to the power of the incoming wave?
 
I agree. But they don't add up :/
 
diracdelta said:
I agree. But they don't add up :/
Please post your working.
 
I got it ;)
Finally.
Thank you very much :)
 

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