Fundamental frequency change because of bouyant force

In summary: I thank you a lot for your great help and replies, at least now I know that there is no hidden third condition to find ##L## and that I only needed to find ##\mu## that I was able to do since the very beginning, but that I did not see I needed to find ##m_{rope}##..Thanks again :!!)In summary, the conversation discussed a problem involving a rope with one end fixed and the other passing through a pulley with a body attached to it. The fundamental frequency of the rope was initially 400 Hz and became 345 Hz when the body was put in water. The linear mass density of the rope was given as 10 g/m and the task was
  • #1
Soren4
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2

Homework Statement


A rope has an end fixed and the other is passing through a pulley and has a body attached to it. The fondamental frequency of the rope is initially ##f_1=400 Hz##. If the body is then put in water the fondamental frequency of the rope becomes ##f_2=345 Hz##. If the linear mass density of the rope is ##\mu=10 g/m## determine
a) the density ##\rho## of the body
b) the length of the horizontal part of the rope ##L##

Homework Equations

The Attempt at a Solution


For point a) I don't have problems since
$$\frac{f_2}{f_1}=\sqrt{\frac{T_1}{T_2}}=\sqrt{\frac{mg-\rho_{H_2O}Vg}{mg}}=\sqrt{\frac{mg-\rho_{H_2O}\frac{m}{\rho}g}{mg}}=\sqrt{1-\frac{\rho_{H_2 O}}{\rho}}$$
Where ##T## is the tension of the rope. From which I can get ##\rho##

But what about point b)?! It seems impossible to me to get ##L## just knowing ##\rho##, ##f_1##, ##f_2## and ##\mu##..
These conditions are not enough, how can I determine ##L##?
 
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  • #3
NascentOxygen said:
Knowing the frequency, can you determine its wavelength, using v=f.λ
http://hyperphysics.phy-astr.gsu.edu/hbase/waves/string.html

Thanks for the answer!

Having the wavelenght would solve the problem because ##\lambda_1=\lambda_2=2L##, the problem is that I cannot have ##v_1## and ##v_2## but only the ratio $$\frac{v_2}{v_1}=\sqrt{\frac{T_2}{T_1}}$$ Which I already used to determine ##\rho##.

Is there another condition I can use to determine ##\lambda##?
 
  • #4
Soren4 said:
Thanks for the answer!

Having the wavelenght would solve the problem because ##\lambda_1=\lambda_2=2L##, the problem is that I cannot have ##v_1## and ##v_2## but only the ratio $$\frac{v_2}{v_1}=\sqrt{\frac{T_2}{T_1}}$$ Which I already used to determine ##\rho##.

Is there another condition I can use to determine ##\lambda##?
There is a piece of information you have not used. There is an equation at the link NascentO posted you can use it in.
 
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  • #5
haruspex said:
There is a piece of information you have not used. There is an equation at the link NascentO posted you can use it in.
Thanks a lot for the reply!

I read all the link and formulas but I fail to see the piece of information I did not use. After all here I have 3 indipendent unknown
  • Lenght of (horizontal part of) the rope ##L##
  • Density of the object ##\rho##
  • Mass of the object ##m## or, equivalently its volume ##V##
The thing is that the tension ##T## depends on both ##m## (for weight) and ##V## (for boyant force), or equivalently on ##m## and ##\rho## or also on ##\rho## and ##V##. But I need two indipendent pieces of information only for tension.

On the other hand the conditions I have are only 2, that is

$$ f_1=\frac{\sqrt{T_1}}{\sqrt{\mu} 2L}=\frac{\sqrt{mg}}{\sqrt{\mu} 2L}\tag{1}$$ $$f_2=\frac{\sqrt{T_2}}{\sqrt{\mu} 2L}=\frac{\sqrt{mg-\rho_{H_20}V g}}{\sqrt{\mu} 2L}\tag{2}$$

And considering 3 indipendent unknowns I really do not know where to get ##L## from.

In the link I found the following formula
$$f=\frac{v}{2L}=\frac{\sqrt{\frac{T}{m_{rope}/L}}}{2L}$$

But here ##m_{rope}## is the mass of the rope which I do not know from data..

Would you be so kind as to suggest me where this not-used piece of information is?
 
  • #6
Soren4 said:
linear mass density of the rope is μ=10g/m

Soren4 said:
I fail to see the piece of information I did not use.
 
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  • #7
Thanks again for the answer! Knowing ##\mu## allows me to get ##L## once I know ##m_{rope}##.

But getting ##m_{rope}## is still a problem, as ##m_{rope}## has nothing to do with the mass of the object ##m##, its volume ##V## or its density ##\rho##.. So it is still an indipendent variable..

I can surely rewrite the equations I have as

$$ f_1=\frac{\sqrt{T_1}}{\sqrt{m_{rope}} 2\sqrt{L}}=\frac{\sqrt{mg}}{\sqrt{m_{rope}} 2\sqrt{L}}\tag{1}$$ $$f_2=\frac{\sqrt{T_2}}{\sqrt{m_{rope}} 2\sqrt{L}}=\frac{\sqrt{mg-\rho_{H_20}V g}}{\sqrt{m_{rope}} 2\sqrt{L}}\tag{2}$$

But these are still 2 equations in 3 variables (##m_{rope}##, ##m## and ##V##).

I really do not know how I cannot see this :headbang:, but it seems to me that the variables are still three and there are just two conditions.. Forgive my incapacity to understand this, if I may ask is there any further clue of the condition to use that you could give me ?
 
  • #8
Soren4 said:
I cannot see this
You are not looking at the right equation. In the link NascentO posted, there is an equation relating velocity, tension and mass per unit length.
 
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  • #9
haruspex said:
You are not looking at the right equation. In the link NascentO posted, there is an equation relating velocity, tension and mass per unit length.

Thanks a lot for your kind help!

The only possible equation in the link relating these variables is $$v=\sqrt{\frac{T}{\mu}}=\sqrt{\frac{T}{m_{rope}/L}}$$ I rewrite the two conditions I have

$$f_1 \cdot 2 L=v_1=\sqrt{\frac{T_1}{\mu}}=\sqrt{\frac{T_1}{m_{rope}/L}}\tag{1}$$
$$f_2 \cdot 2L=v_2=\sqrt{\frac{T_2}{\mu}}=\sqrt{\frac{T_2}{m_{rope}/L}}\tag{2}$$

Again 2 equations and 3 indipendent unknowns (##T_1##, ##T_2##, ##L##) :cry:

This allows me only to find the following ratios (where ##L##, or ##m_{rope}## disappear, as they are equal for both cases)

$$\frac{v_1}{v_2}=\frac{f_1}{f_2}=\sqrt{\frac{T_1}{T_2}}$$

I tried to use ##\mu## as suggested but it does not give a further indipendent condition

I'm sorry to ask again, but apparently this simple exercise is really driving me crazy in finding this hidden third condition... What use of eq ##v=\sqrt{\frac{T}{\mu}}## and of ##\mu## should I do?
 
  • #10
Soren4. I'm with you, I don't think there's enough info to find L.
 
  • #11
TSny said:
Soren4. I'm with you, I don't think there's enough info to find L.
Yes, I'm sorry - I just assumed that because you had not used the value of μ it must be possible to deduce more. But you are quite right, there's not enough information.
Sorry ro have wasted your effort on this.
 
  • #12
Soren4 said:
But what about point b)?! It seems impossible to me to get ##L## just knowing ##\rho##, ##f_1##, ##f_2## and ##\mu##..
These conditions are not enough, how can I determine ##L##?
Missing data? I hadn't noticed that. Do you have the textbook's answer for L? If so, we could work backwards and determine what's missing...perhaps they intended that you be told the volume of the body to be submerged, e.g., 10 litres.

There's a tiny video clip here that illustrates the change in wave velocity. He uses the rung of a ladder as the pulley from which to hang weights, and then counts each reflection as the wave returns.
 

1. What is the fundamental frequency?

The fundamental frequency is the lowest frequency at which a system can vibrate. It is the natural frequency of an object or system, and it determines the pitch of a sound.

2. How does buoyant force affect the fundamental frequency?

Buoyant force is the upward force exerted on an object immersed in a fluid. This force can change the effective mass and stiffness of an object, which in turn affects its fundamental frequency.

3. Can buoyant force increase the fundamental frequency?

Yes, buoyant force can increase the fundamental frequency of an object. This is because the added upward force decreases the effective mass of the object, making it vibrate at a higher frequency.

4. How does the density of the fluid affect the fundamental frequency change?

The density of the fluid plays a significant role in the magnitude of the fundamental frequency change due to buoyant force. A denser fluid will exert a greater upward force on an object, resulting in a larger change in the fundamental frequency.

5. Is the change in fundamental frequency due to buoyant force always significant?

The change in fundamental frequency due to buoyant force can vary depending on factors such as the density of the fluid, size and shape of the object, and the location of the object in the fluid. In some cases, the change may be minimal and not noticeable, while in others it can be significant and easily detectable.

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