Density and simple harmonic motion

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Homework Help Overview

The problem involves a mass of density d floating in a liquid of density d_L, which is pushed down a distance x and released. The objective is to demonstrate that the mass undergoes simple harmonic motion using Newton's Second Law, while also recalling the SHM equation and finding the angular frequency w in terms of relevant variables.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of Newton's Second Law and the relevance of torque in the context of the problem. Some suggest starting with a free body diagram to analyze forces acting on the mass. Questions arise regarding the role of torque and its application in this scenario.

Discussion Status

The discussion includes various attempts to relate forces and torques to the motion of the mass. Some participants express confusion about how to connect their findings to the concept of simple harmonic motion. There is a shift towards focusing on the forces involved and their equations, with one participant indicating they have resolved their confusion by the end of the discussion.

Contextual Notes

Participants are working under the assumption that there is no friction and are exploring the implications of the forces acting on the mass in relation to its motion. The problem context suggests a need for clarity on the definitions and roles of forces in this specific setup.

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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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