Simple Harmonic Motion, object floating in a liquid

In summary, the problem asks to show that the period of small oscillations of a body floating in a liquid is given by \tau = 2\pi \sqrt{V/gA}, and to determine the value of \tau. The attempt at a solution involves finding an equation for the restoring force in terms of mgA and V, but the attempt leads to Apg instead of mgA/V. The solution is trivial as p=m/V by definition.
  • #1
Jack21222
212
1
(apologies for the formatting, mixing LaTeX and regular text looks ugly, but I don't know how to do it otherwise)

Homework Statement



This is problem 3-7 from Thornton and Marion's Classical Dynamics.

A body of uniform cross-sectional area A = 1 cm2 and of mass density [tex]\rho[/tex]=0.8 g/cm3 floats in a liquid of density [tex]\rho[/tex]0=1 g/cm3 and at equilibrium displaces a volume V = 0.8 cm3. Show that the peroid of small oscillations about the equilibrium position is given by:

[tex]\tau[/tex] = 2[tex]\pi[/tex] [tex]\sqrt{V/gA}[/tex]

where g is the gravitational field strength. Determine the value of [tex]\tau[/tex]

Homework Equations



[tex]\tau[/tex] = 2[tex]\pi[/tex][tex]\sqrt{k/m}[/tex] (equation 3.13 in the book)

k[tex]\equiv[/tex] -(dF/dx)

The Attempt at a Solution



It appears to me that if I can show V/gA = m/k or k = mgA/V, then the equation in the problem would be equal to equation 3.13 quoted above. I tried coming up with an equation for the restoring force F in terms of mg A and V, and then take the x-derivative of k, but it doesn't equal mgA/V.

I'll be using p = rho from here, because I don't want to mix LaTeX and regular text, and p has no other meaning.

The restoring force I came up with was F = Vp0g - mg where m is the mass of the block.

In terms of x, I get F = Axpg - mg where x is the depth of the submerged block.

Taking the x-derivative of F, from the definition of k, I get Apg, which isn't equal to mgA/V

Any suggestions?
 
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  • #2
I'm an idiot, p= m/V by definition, and everything falls together.

I can't believe I got stuck on such a trivial step. I'm embarrassed that I even posted this thread.
 

FAQ: Simple Harmonic Motion, object floating in a liquid

What is Simple Harmonic Motion?

Simple Harmonic Motion (SHM) is a type of periodic motion in which the restoring force is directly proportional to the displacement of the object from its equilibrium position. This means that the object moves back and forth in a regular pattern around its equilibrium point.

How is Simple Harmonic Motion related to an object floating in a liquid?

When an object is floating in a liquid, it is subject to the force of gravity pulling it down and the buoyant force of the liquid pushing it up. If the object is displaced from its equilibrium position, it will experience a restoring force that is proportional to its displacement, just like in SHM.

What factors affect the frequency of Simple Harmonic Motion in an object floating in a liquid?

The frequency of SHM in an object floating in a liquid depends on the mass of the object, the stiffness of the liquid, and the depth at which the object is floating. A heavier object or a stiffer liquid will have a higher frequency, while a deeper depth will have a lower frequency.

Can the amplitude of Simple Harmonic Motion in an object floating in a liquid change over time?

Yes, the amplitude of SHM can change over time in an object floating in a liquid. This can happen due to changes in the properties of the liquid, such as temperature or salinity, or if the object is affected by external forces like waves or currents.

What is the equation for calculating the period of Simple Harmonic Motion in an object floating in a liquid?

The period, or time for one complete cycle, of SHM in an object floating in a liquid is given by the equation T = 2π√(m/k), where T is the period, m is the mass of the object, and k is the stiffness of the liquid.

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