Ate of energy transfer by sinusoidal waves on a string q

AI Thread Summary
The discussion focuses on demonstrating that the amplitude A of a two-dimensional water wave at a distance r from the initial disturbance is proportional to 1/√r. Participants emphasize the importance of considering the energy carried by outward-moving ripples, noting that energy is proportional to A². As the wave spreads in a circular pattern, the energy is distributed over the circumference of the wave front, which is πr. This relationship helps establish the inverse square root dependence of amplitude on distance. Understanding these principles is crucial for solving the problem effectively.
lizzyb
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Q: A two-dimensional water wave spreads in circular wave fonts. Show that the aplitude A at a distance r from the initial disturbance is proportional to \frac{1}{\sqrt{r}}. (Hint: Consider the energy carried by one outward moving ripple.)

Comments:
Let's consider the energy carried by one outward-moving ripple:
E_\lambda = \frac{1}{2} \mu \omega^2 A^2 \lambda
and I suppose there is another wave directly across the origin for some particle. But how do I relate this to r?

thanks!
 
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Consider the energy density of the ripple. That is the energy per unit length. The length of the wave being a circle is \pi r and then consider the equation you have given above for energy as it contains the amplitude.
 
lizzyb said:
Q: A two-dimensional water wave spreads in circular wave fonts. Show that the aplitude A at a distance r from the initial disturbance is proportional to \frac{1}{\sqrt{r}}. (Hint: Consider the energy carried by one outward moving ripple.)

Comments:
Let's consider the energy carried by one outward-moving ripple:
E_\lambda = \frac{1}{2} \mu \omega^2 A^2 \lambda
and I suppose there is another wave directly across the origin for some particle. But how do I relate this to r?

thanks!
All you really need to know to do this problem is that the energy is proportional to A². Since the wave is spreading out in a circle, the energy is being spread over the curcumference of the wave front.
 
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