What is the period of a bobbing cork?

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The discussion centers on calculating the period of oscillation for a cork floating in water, given its dimensions and density. The user calculated the mass of the cork and set up a differential equation to analyze the forces acting on it, including restoring and gravitational forces. There is confusion regarding the correct formulation of the equation and the method to find the period, with suggestions to redefine the displacement variable for clarity. Participants emphasize understanding the equilibrium forces and comparing the system to a vertical spring to simplify the analysis. The goal is to accurately determine the period of oscillation, which the user initially calculated as 0.859 seconds but found to be incorrect.
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Homework Statement



A cork floats in water. The cork is a cylinder with radius 1 cm and height 3.4 cm. The density of the cork is 0.55 g/cc. Calculate the period of oscillation if the cork is pushed down a little and released.

Homework Equations



I think I need help with the restoring force... please.

The Attempt at a Solution



-1st I found the mass of the cork - M=D*V =
D = (.55g/cm3)*(1kg/1000g)*(100cm/m)3 = 550kg/m3
V = pi*r2*h = pi*(.01m)2*.034m = 1.068E-5 m3

M = 550kg/m3*1.068E-5m3 = 5.874E-3 kg

-Then setting up my differential:
Fnet = Frestore + Fgravity

Fr = -Dh2o*Vh2o : (Density of water * volume of water displaced)

Fg = mg

ma = mg - Dh2o*Vh2o

volume is dependent on y, or the height, so V = pi*r2*y

-rearranging the equation my'' + Dh2o*pi*r2*y = mg

divide by m --> y'' + Dh2o*pi*r2*y/m = g

and setting y=ert

r1=+isqrt(Dh2o*pi*r2*/m)
r2=-isqrt(Dh2o*pi*r2*/m)

I don't need the particular solution because we need to calculate the period, and

y(t) = Acos{sqrt(Dh2o*pi*r2*/m)t}
+ Bsin{sqrt(Dh2o*pi*r2*/m)t}

the period should be 2*pi/(sqrt(Dh2o*pi*r2*/m) right?

I got .859s but this is not correct. If anyone has some advice, I would be much obliged.
 
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I would first suggest to redefine y so that y=0 when the cork is at equilibrium. Then, you a have a VERY popular (in physics) type of 2nd order diff. eq., from which you can directly read off the frequency. Actually, it is not really necessary to redefine y, but I think it might make the equation easier for you to recognize.

BTW, y=e^rt is certainly not correct.
 
turin said:
I would first suggest to redefine y so that y=0 when the cork is at equilibrium. Then, you a have a VERY popular (in physics) type of 2nd order diff. eq., from which you can directly read off the frequency. Actually, it is not really necessary to redefine y, but I think it might make the equation easier for you to recognize.

BTW, y=e^rt is certainly not correct.

Try phrasing the restoring force as a force of the form \vec F(y) = -C\vec y, and think about what that says about the system.
A good way to start is to look at what the net force on the cork is at equilibrium, and what it is when you've displaced it by a height of y into the water (Remember that the force mg doesn't change).

A good mental analogy to make in this case would be comparing it to a vertical spring, I assume you've already dealt with that problem, try and remember how you dealt with the effect of gravity there, it's very similar here.
 
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