Ratio of µ in a rope with differing thickness/Waves

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In summary: L_left/µ_left)/(Γ/2µ_right)Simplifying this equation, we get:µ_left/µ_right = 4L_left/Γ_rightIn summary, the ratio of µ for the different sections is equal to 4 times the length of the left section divided by the amplitude of the transmitted pulse on the right.
  • #1
gmmstr827
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Homework Statement



For the cord in the following diagram, what is the ratio of µ for the different sections to create a Γ/2 on the right?

*** The picture depicts a rope with an upward oriented reflected pulse on the left (thinner rope) and a downward oriented transmitted pulse on the right (thicker rope). ***
http://i29.photobucket.com/albums/c261/gmmstr827/rope.jpg

Homework Equations



Useful formulas might include:
Γ = v/f
Γ_n = 2L/n where n=1 represents 1st harmony; n=2 represents 2nd harmony, etc.
v = velocity
f = frequency = 1/T
T = period = 2π√(L/g)
g = 9.8 m/s^2
L = length
µ = m/L
m = mass

The Attempt at a Solution



Perhaps if you solve Γ_n = 2L/n where n=1 for L = Γ/2 then plug that into L in µ = m/L to get µ = (mΓ)/(2L) that could be your ratio?

It seems like the answer would be that the rope on the right is twice the µ than the rope on the left, however I'm unsure how to show this. There don't seem to be many connections between the formulas for µ and Γ for this to easily be solved. If someone could guide me to the correct formulas, it would make this much easier. Thank you!
 
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  • #2

Thank you for your question. I would like to help you find the correct solution to this problem.

To start, let's define some variables:
- Γ: the amplitude of the reflected pulse (upward oriented) on the left side of the rope
- Γ/2: the amplitude of the transmitted pulse (downward oriented) on the right side of the rope
- L: the length of the rope
- µ: the linear density of the rope
- m: the mass of the rope
- n: the harmonic number

From the given formulas, we can see that Γ = v/f. This means that the amplitude of the reflected pulse is equal to the velocity divided by the frequency. We also know that the frequency is equal to 1/T, where T is the period. The period can be calculated using T = 2π√(L/g), where g is the acceleration due to gravity. Therefore, we can rewrite the formula for Γ as Γ = v/(1/T) = vT.

Next, let's look at the formula for Γ_n = 2L/n. This formula tells us that the amplitude of the nth harmonic is equal to 2L divided by the harmonic number. In this case, we are interested in the first harmonic (n=1), which corresponds to the reflected pulse on the left side of the rope. So, we can rewrite this formula as Γ = 2L/1 = 2L.

Now, let's combine these two formulas for Γ:
Γ = vT = 2L

We can also use the formula for µ = m/L to calculate the linear density of the rope. Since we are looking for the ratio of µ for the different sections, we can set up the following equation:
µ_left/µ_right = (m_left/L_left)/(m_right/L_right)

We know that the mass of the rope is equal to its linear density multiplied by its length, so we can rewrite this equation as:
µ_left/µ_right = (m_left/µ_left)/(m_right/µ_right)

We also know that the mass is directly proportional to the amplitude of the pulse, so we can rewrite this equation as:
µ_left/µ_right = (Γ_left/µ_left)/(Γ_right/µ_right)

Now, we can substitute the formulas for Γ_left and Γ_right into this equation:
µ_left/µ
 

Related to Ratio of µ in a rope with differing thickness/Waves

1. What is the ratio of µ in a rope with differing thickness?

The ratio of µ (the coefficient of friction) in a rope with differing thickness will depend on the material of the rope and the surface it is rubbing against. The thicker the rope, the more surface area there is to create friction, thus increasing the µ value.

2. How does the thickness of a rope affect the ratio of µ?

The thickness of a rope can directly affect the ratio of µ. As mentioned earlier, a thicker rope will have more surface area to create friction, resulting in a higher µ value. However, if the rope is too thin, it may not have enough contact with the surface to create significant friction.

3. Can the ratio of µ change with different types of waves?

Yes, the ratio of µ can change with different types of waves. The type of wave, such as transverse or longitudinal, can affect the movement and interaction of the rope, thus impacting the µ value.

4. How can the ratio of µ be measured in a rope with differing thickness and waves?

The ratio of µ can be measured using a variety of techniques such as using a force sensor to measure the force required to move the rope, or using a dynamometer to measure the tension in the rope. These measurements can then be used to calculate the µ value.

5. Are there any other factors that can affect the ratio of µ in a rope?

Yes, there are other factors that can affect the ratio of µ in a rope, such as the surface roughness of the rope and the surface it is interacting with, the angle at which the rope is pulled, and the speed at which the rope is moving. These factors can all influence the friction between the rope and surface, thus affecting the µ value.

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