Gravitation and Archimedes principle as a spring?

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Homework Help Overview

The discussion revolves around the interplay of gravitational forces and Archimedes' principle in the context of a submerged cylinder, exploring the potential energy associated with these forces as analogous to a spring system. Participants are attempting to derive a spring constant 'K' and understand its relationship to the forces acting on the cylinder.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants are discussing how to express the potential energy of a system involving gravitational and buoyant forces in terms of a spring constant. There are attempts to derive the relationship between these forces and the spring constant 'K', with questions about the algebra involved and the nature of 'K' as potentially variable or constant.

Discussion Status

There is an ongoing exploration of the equations governing the system, with some participants suggesting potential forms for 'K' and its implications for potential energy. The discussion is dynamic, with various interpretations and approaches being considered, but no consensus has been reached on the final form of the equations or the value of 'K'.

Contextual Notes

Participants are working under the assumption that the system is in equilibrium and are questioning how to incorporate the displacement into their equations. There is also a recognition that the potential energy expression may need to account for a new equilibrium position.

uriwolln
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Hey all,

I have seen that these two forces combined together have the potential energy of a spring with a constant 'K' as a combination of some sort of the two forces.
I have no idea how am I to find this K.
All I know
Mgh + ρVgh gives the potential energy of a given system let's say.

help?
 
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uriwolln said:
Hey all,

I have seen that these two forces combined together have the potential energy of a spring with a constant 'K' as a combination of some sort of the two forces.
I have no idea how am I to find this K.
All I know
Mgh + ρVgh gives the potential energy of a given system let's say.

help?

Can you try to re-phrase what you are having difficulty with please?
 
The problem was:
A cylinder is placed inside water, and it is in equilibrium when half of the cylinder height is submerged. So I Know there is the archimedes principle which causes a force upwards and then there is gravity downwards. This problem was part of question somewhere, but in the explanation of the answer concerning the energies of the system when it is in motion, they somehow did not use mgh of either the ρVgh. They did a combination of those to act as a spring, which I did not get a clear answer on how to do that.
 
hi uriwolln! :smile:

if the restoring force is proportional to the distance from the equilibrium position,

the the equation is exactly the same as the equation for a spring :wink:
 
:)
Did not think of it this way.
But then, what will be 'k' equal to?
How do I work the algebra for it?
and will the potential energy of it all will indeed be k(x^2)/2?
 
uriwolln said:
But then, what will be 'k' equal to?
How do I work the algebra for it?

try it and see :wink:
 
So let's see:
kx=mg - ρVg ==> k = (mg - ρVg)/2 ?
and then potential energy: k(x^2)/2?
 
uriwolln said:
kx=mg - ρVg

but V depends on x :redface:
 
:)
true... forgot that for a sec... but is this the equation I should go for?
K being a function of x? Then the whole potential energy is going wrong, because K is not constant, or does it? ( I think K should be constant to use k(x^2)/2)
 
  • #10
erm :redface: … first, find the equation

then analyse it! :wink:
 
  • #11
Here goes:

Kx = (pir2H)g - ρ(pir2(H-x)g/2)
K = (pir2Hg/2x) + ρ(pir2g)/2
 
  • #12
uriwolln said:
Kx = …

no, you mean mx'' = …

carry on from there :wink:
 
  • #13
mx?
why am I meaning mx? m as in mass? and x as displacement?
Then where does K come in?

(I am not being disrespectful I hope, I really liked your comment, which made me laugh, because I really do not know why should I use mx)
 
  • #14
no, mx''

(ie md2x/dt2)
 
  • #15
:)
ρcpir2Hx'' = ρcpir2Hg - ρl(pir2(H/2 - x)
x'' + x(ρlg/ρcH) = g(1-ρl/2ρc)
Which x then I know is oscillating.
But then where does K come in?
 
  • #16
uriwolln said:
x'' + x(ρlg/ρcH) = g(1-ρl/2ρc)

you have x'' = -Ax + B

if it was just x'' = -Ax, what would k be? :wink:
 
  • #17
then K should be:
k = (ρlg/ρcH)
So potential energy is as well 0.5Kx2?
 
  • #18
uriwolln said:
then K should be:
k = (ρlg/ρcH)

yes :smile:, but I'm not sure whether you're just guessing :wink:

how did you get rid of the B?
So potential energy is as well 0.5Kx2?

maybe … what's x?
 
  • #19
:)
actually I did guess.
Well, I mean, I figured because it was the coefficient of x, then it would be reasonable to assume that, that is K.
X would be the answer for the differential equation I got previous.
 
  • #20
uriwolln said:
:)
actually I did guess.

:biggrin:
Well, I mean, I figured because it was the coefficient of x, then it would be reasonable to assume that, that is K.

ok, sensible guess for k :smile:, but it doesn't tell you how to combine it with the distance (in kx or 1/2 kx2) :redface:

when you have x'' = -Ax + B,

rewrite that as (x - B/A)'' - -A(x - B/A) …

now you have it in the same form as the standard spring equation :wink:
 
  • #21
AWESOME!
Thanks for that.
Tell me please though, if I did write x to be x - B/A then I think I should be using x - B/A for the potential energy as the x there: 0.5Kx^2. Correct?
 
  • #22
Correct. :smile:

x = B/A is the equilibrium position, and all displacements must be measured from that.

(you get the same effect if you take a horizontal spring and place it vertically, with a weight on the end … the new equilibrium position is different from the original equilibrium position, and all displacements must be measured from the new position instead)
 
  • #23
:)
Thank you so much tiny!
 

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