Density and simple harmonic motion

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SUMMARY

The discussion centers on demonstrating that a mass of density d, floating in a liquid of density d_L, undergoes simple harmonic motion (SHM) when displaced and released. Using Newton's Second Law, the equation of motion is derived, leading to the conclusion that the angular frequency w is given by w = SQRT(d_L * g / (d * H)). The participants clarify the roles of buoyant force and gravitational force in the system, ultimately confirming that the mass will oscillate in SHM without friction.

PREREQUISITES
  • Understanding of Newton's Second Law (F = ma)
  • Knowledge of buoyant force principles
  • Familiarity with simple harmonic motion equations
  • Basic concepts of torque and rotational dynamics
NEXT STEPS
  • Study the derivation of the simple harmonic motion equation d^2x/dt^2 + w^2*x = 0
  • Explore the relationship between density, buoyancy, and oscillation frequency
  • Learn about free body diagrams and their application in dynamics problems
  • Investigate the effects of friction on simple harmonic motion
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators looking for examples of simple harmonic motion applications.

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Homework Statement


A mass of density d floats in a liquid of density d_L. The mass is then pushed down a distance x and let go. Use Newton's Second Law to demonstrate that the mass will undergo simple harmonic motion. Recall that the SHM equation is d^2x/dt^2 + w^2*x = 0. Assume there is no friction. Find w in terms of whatever variables needed.


Homework Equations





The Attempt at a Solution



I know that Newton's 2nd law is sum F=ma, and Torque = I*omega. I don't see how I can relate this to simple harmonic motion, which involves things moving back and forth in the same pattern. The answer key says that w=SQRT(D_l * g/(D*H)). However, I don't know what I am missing to solve this problem. I don't know where to start.
 
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I think a free body diagram would be a good place to start. Then I would use Newton's second law. Torque, huh?
 
When the object is at rest, I have mg pulling down and buoyant force pushing up. They are equal in magnitude. The net torque is also zero.

When the object is pushed down I have f pushing down, mg pulling down, and buoyant force pushing up. This extra f is enough to push it down. My net torque is

T = IW

However, why would I use this? Isn't torque normally used when things are rotated?

T = F x R

What R in this case? Mg and buoyant are both pushing from the center in the free body diagram so I don't think there is an R. So f is the only force that contributes to the torque am I correct?
 
Torque shouldn't come into play. You've listed some forces, now put them into equations.
 
For the object at rest

I got

B - mg = 0

When it's pushed down

B - mg -f = -ma

Since B =mg

f = ma

I already know this though so how does it help prove that it's in simple harmonic motion with a repeating pattern?
 
Never mind I got it now. Thanks a lot for your help.
 

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