Solving for Maximum Speed of Cube: Kinematics & Upthrust

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Homework Help Overview

The discussion revolves around a kinematics problem involving a cube and the forces acting on it, specifically focusing on upthrust and gravitational forces. Participants are exploring how to determine the maximum speed of the cube after a string is cut, considering the effects of acceleration and energy conservation.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants are examining the relationship between forces acting on the cube and its acceleration, with one suggesting the use of energy conservation instead of kinematics due to the non-constant acceleration. There are discussions about the initial and final energy states, including gravitational potential energy (GPE) and kinetic energy (KE). Others are questioning the integration of differential equations related to the motion of the cube.

Discussion Status

The conversation is active, with various interpretations of the problem being explored. Some participants are providing guidance on using energy methods and differential equations, while others are seeking clarification on the equations and their implications. There is no explicit consensus yet, as participants are still questioning and refining their understanding of the problem.

Contextual Notes

Participants are navigating the complexities of the problem, including the need to account for the water's GPE and the nature of the differential equations involved. There is an acknowledgment of the limitations of certain kinematic equations in this context.

jisbon
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Homework Statement
1) Cube is initially attached to string on the bottom of a container filled with water
2) The density of cube is half of the density of water
3) The surface of the water is same level of the top surface of the cube
4) The density of water is p
What is the largest speed of cube when travelling upward after cutting the string?
Relevant Equations
-
So, I recognise that:

$$ma=pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3} $$
whereby $$pg\left( L^{2}\right) \left( L-y\right)$$ is the upthrust while the other is mg.

So, to find the largest speed of cube, I will assume that acceleration is zero since the acceleration slowly decreases after I cut the string (as mg = upthrust)
So, I should take a=0
I found a to be :
$$\dfrac {pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3}}{m} $$
and y= 1/2L after making the upthrust and mg equals
So using kinematics, I should be able to find v with :
$$v^2=u^2+2as$$
where a is what I found above and s to be 1/2 L. However, the answer comes out as 0.
Not sure what happened here :/
Thanks
 
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jisbon said:
So using kinematics,
The equation you quote is only valid for constant acceleration.
You could use energy.
 
haruspex said:
The equation you quote is only valid for constant acceleration.
You could use energy.
What will be the energy involved in this case though?
Initial energy = gpe? Final energy = gpe+ ke?
Thanks
 
jisbon said:
What will be the energy involved in this case though?
Initial energy = gpe? Final energy = gpe+ ke?
Thanks
Yes. Remember to take into account the water's GPE.
An alternative is to solve the differential equation you had for y.
 
haruspex said:
Yes. Remember to take into account the water's GPE.
An alternative is to solve the differential equation you had for y.
By differential equation for y, do you mean integrating $$\dfrac {pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3}}{m}$$ in terms of t?
 
jisbon said:
By differential equation for y, do you mean integrating $$\dfrac {pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3}}{m}$$ in terms of t?
No, you clearly cannot do that. I mean solving the differential equation of which that forms part:
$$\ddot y=\dfrac {pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3}}{m}$$

You may recognise that as a well known form of equation in mechanics.
 
haruspex said:
No, you clearly cannot do that. I mean solving the differential equation of which that forms part:
$$\ddot y=\dfrac {pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3}}{m}$$

You may recognise that as a well known form of equation in mechanics.
I'm sorry, but I can't seem to recognise any equations here. Do you mean solving
$$ma = {pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3}}$$
 
jisbon said:
I'm sorry, but I can't seem to recognise any equations here. Do you mean solving
$$ma = {pg\left( L^{2}\right) \left( L-y\right) -\dfrac {1}{2}pgL^{3}}$$
Yes, but a is the same as ##\ddot y##, and the nature of the equation is more obvious in that form. To make it more obvious still, we can collapse various groups of constants into single items:
##\ddot y +Ay+B=0##.
And to make it blindingly obvious, substitute z=y+B/A:
##\ddot z +Az=0##.
 

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