Wave Propagation in a Hanging Rope: Time for Reflection and Return

In summary, a uniform rope of length L and negligible stiffness is hanging from a solid fixture in the ceiling. The free lower end of the rope is struck sharply at time t=0 and the question is asked about the time t it takes for the resulting wave on the rope to travel to the ceiling, be reflected, and return to the lower end of the rope. The equation for wave motion is given as y(t) = A cos(kt-w) for some constants k and w. The velocity of the wave is constant, as determined by the equation v = sqrt(gL). However, in this case, F (tension) is not a constant as each part of the rope is being stretched differently depending on its distance from the
  • #1
wayfarer
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Homework Statement


A uniform rope of length L and negligible stiffness hangs from a solid fixture in the ceiling
The free lower end of the rope is struck sharply at time t=0. What is the time t it takes the resulting wave on the rope to travel to the ceiling, be reflected, and return to the lower end of the rope?

Homework Equations



Equation for wave motion - is it this:
y(t ) = A cos (kt - w),
for some constants k,w.

The Attempt at a Solution


v = sqrt (F/u) = sqrt (mg/ (m/L) ) = sqrt (gL)
this implies that velocity is constant for the wave. I was wondering if this was correct, since it looks suspicious.
From here, I'm not exactly sure where to go - which wave equation should I use to go further (to solve and find out what I want to find out?). Would plugging into the equation I had before, y( t) = A cos(kt-w), be the way to go?
 
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  • #2
F is not a constant in this case, each part of the rope is beeing stretched differently depending on how close it is to the ceiling
 
  • #3
In that case, how would I deal with a situation where F is not constant? I have only learned so far how to deal with cases where it is constant.
 
  • #4
the equation for v is still valid you just have to write F in terms of x (where x is distance from the bottom part of the rope)
 
  • #5
You'll need to integrate. Find the speed of the wave as a function of position along the rope. (What's the tension as a function of position?)
 

FAQ: Wave Propagation in a Hanging Rope: Time for Reflection and Return

What is a "wave through uniform rope"?

A wave through uniform rope refers to a type of mechanical wave that travels through a rope or string with a consistent density and tension. These waves can be created by a disturbance at one end of the rope, and they propagate through the entire length of the rope.

How does a wave travel through a uniform rope?

When a force is applied to one end of the rope, it creates a disturbance in the rope. This disturbance causes the particles of the rope to vibrate, transferring energy from one particle to the next. As the particles vibrate, they create a wave that travels along the rope, carrying the energy with it.

What factors affect the speed of a wave through a uniform rope?

The speed of a wave through a uniform rope is determined by the tension and density of the rope. As the tension increases, the speed of the wave also increases. Similarly, as the density of the rope increases, the speed of the wave decreases.

Can a wave travel through a rope without tension?

No, a wave cannot travel through a rope without tension. The tension in the rope is necessary to create the disturbance that leads to the formation of a wave. Without tension, the particles of the rope would not vibrate and the wave would not be able to propagate.

What are some real-life examples of a "wave through uniform rope"?

One common example of a wave through a uniform rope is when you create a wave by shaking one end of a jump rope. Another example is the movement of sound waves through guitar strings or other musical instruments. Waves through uniform rope can also be seen in the movement of ocean waves or seismic waves through the Earth's crust.

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