Oscillation of a particle on a parabolic surface [equation of motion]

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Homework Help Overview

The discussion revolves around the motion of a particle constrained to move on a parabolic surface described by the equation $$y = Ax^2$$. Participants are tasked with deriving the frequency of oscillation, expressed as $$\omega = \sqrt{2Ag}$$, and are exploring the appropriate coordinate systems and methods to analyze the problem.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the use of Cartesian coordinates and the potential for energy methods. There are attempts to relate kinetic and potential energy, and questions arise about the appropriate equations of motion and the contributions of different components of kinetic energy.

Discussion Status

The conversation is ongoing, with various approaches being explored, including energy conservation and dimensional analysis. Some participants have offered insights into the relationships between variables, while others express uncertainty about their reasoning and calculations. There is no explicit consensus yet on the correct approach or solution.

Contextual Notes

Participants are grappling with the implications of the parabolic shape on the equations of motion and the potential for harmonic motion. There is a recognition of the need for clarity in the relationships between the variables involved, particularly regarding the derivatives and their physical meanings.

happyparticle
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Homework Statement
equation of motion
Relevant Equations
F = ma
##\ddot{\theta} + \frac{k}{m} x = 0##
Hi,

I have a particle on a parabolic surface $$y = Ax^2$$ and I have to show that the frequency is $$\omega = \sqrt{2Ag}$$

I don't know how to deal with a parabola. I don't think I can use the polar coordinates like a circle.

I don't see how to start this problem and in which coordinates system.

For a circle I can use the polar coordinates and then use ##F = ma => -mg sin \theta = mR\ddot{\omega}##

I have to get the equation of motion $$\ddot{\theta} + 2Ag \theta = 0$$

thus, ##2Ag = \omega^2##
 
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EpselonZero said:
which coordinates system.
It’s straightforward enough in Cartesian.
Draw a diagram of the particle at some (x,y) and analyse the forces.
 
I think using energy ##u(y) = mgy## can get the job done. Someone pointed out to me. I didn't notice.

However, is it the only way?
 
EpselonZero said:
I think using energy ##u(y) = mgy## can get the job done.
What about KE?
 
haruspex said:
What about KE?
##y_{max}, E = mgy_{max}##

##K = E - U, \frac{1}{2}m\dot{x}^2 = mgy_{max} - mgy##

##\dot{x} = \sqrt{2g(y_{max} - Ax^2)}##

I'm stuck here, Am I in the right path?

I'm wondering if ##y_{max} = Ax_{max}^2##
 
EpselonZero said:
##\frac{1}{2}m\dot{x}^2 = mgy_{max} - mgy##
What about ##\dot y##?
 
haruspex said:
What about ##\dot y##?
##\dot{y} = 2A\dot{x}##

##\dot{x} = \frac{\sqrt{2g}}{2A}##

That doesn't work and I can find why.
 
EpselonZero said:
##\dot{y} = 2A\dot{x}##

##\dot{x} = \frac{\sqrt{2g}}{2A}##

That doesn't work and I can find why.
No, I mean as part of the KE.
 
haruspex said:
No, I mean as part of the KE.
That's what I did.

##2A\dot{x} =\sqrt{2g} (y_{max} - y)##

##\dot{x} = \frac{\sqrt{2g}}{2A}(y_{max} - y)##
 
  • #10
EpselonZero said:
##\dot{y} = 2A\dot{x}##
That equation is wrong. You have not differentiated x2 correctly. Use the chain rule.
EpselonZero said:
##\frac{1}{2}m\dot{x}^2 = mgy_{max} - mgy##
That equation is wrong because it omits the KE embodied in the vertical component of motion.
 
  • #11
If ## \frac{1}{2}m\dot{y}^2 = mgy_{max} - mgy##

I get ##x = \frac{\sqrt{2g}}{2A}(y_{max} - y)##

or ##\dot{y} = \sqrt{2g}(y_{max} - y)##
 
  • #12
EpselonZero said:
If ## \frac{1}{2}m\dot{y}^2 = mgy_{max} - mgy##
Now you are only counting the vertical component of KE. Both contribute.
 
  • #13
haruspex said:
Now you are only counting the vertical component of KE. Both contribute.
Ah, I see, but how I do that.
##K = \frac{1}{2}m\dot{y}^2 + \frac{1}{2}m\dot{x}^2##

##U = mgy##

##E = mgy_{max} + mgx_{max}##Which gives me

##\dot{y}^2 + \dot{x}^2 = 2g(y_{max} + x_{max} - y)##

I'm not sure what to do with the left side.
 
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  • #14
EpselonZero said:
##E = mgy_{max} + myx_{max}##
I assume you meant mgxmax, but I don't understand the reason for that term. What aspect of GPE is not covered by mgy?
 
Last edited:
  • #15
E = total energy

When the particle is at ##y_{max}## then all the energy = U, thus ## E = mgy_{max}##
 
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  • #16
EpselonZero said:
E = total energy

When the particle is at ##y_{max}## then all the energy = U, thus ## E = mgy_{max}##
Sorry, missed out a crucial word ("not") in post #14.
So, yes, ## E = mgy_{max}##.

What dynamic energy equation does that give you (instead of the one at the end of post #13), and what equation connects ##\dot y, \dot x## ( it is not ##\dot y=2A\dot x##)?
 
  • #17
haruspex said:
What dynamic energy equation does that give you (instead of the one at the end of post #13), and what equation connects ##\dot y, \dot x## ( it is not ##\dot y=2A\dot x##)?

## \dot{y}^2 + \dot{x}^2 = 2g(y_{max} - y)##

##\dot{y} = 2Ax##

##\dot{x} = \frac{1}{2\sqrt{A}\sqrt{y}}##

sorry, I can't find a connection between ##\dot{x},\dot{y}##
 
  • #18
EpselonZero said:
##\dot{y} = 2Ax##
sorry, I can't find a connection between ##\dot{x},\dot{y}##
That equation is wrong. You have differentiated the LHS wrt t but the RHS wrt x. How do you differentiate Ax2 wrt t?
The relationship I am asking for is the correct form of that.
 
  • #19
I'm sorry...
##\dot{y} = A\dot{x}^2##

##\dot{y}^2 + \frac{\dot{y}}{A} = 2g(y_{max} - y)##

I can't have ##\sqrt{2Ag}##
 
  • #20
EpselonZero said:
I'm sorry...
##\dot{y} = A\dot{x}^2##
Still wrong.
Use the chain rule.
 
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  • #21
A is a constant
##\frac{dy}{dt} = A \frac{d(x^2)}{dt}##
 
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  • #22
EpselonZero said:
A is a constant
##\frac{dy}{dt} = A \frac{d(x^2)}{dt}##
Yes, but what do you get when you apply the chain rule to the RHS?
You've so far tried ##2Ax## and ##A\dot x^2##.
(You are familiar with the chain rule?)
 
  • #23
haruspex said:
(You are familiar with the chain rule?)

I think so, but I don't see how to use the chain rule here.
I mean, I can use the chain rule if I have something like ##\sqrt{(x^2y-xy)}##
 
  • #24
EpselonZero said:
I think so, but I don't see how to use the chain rule here.
I mean, I can use the chain rule if I have something like ##\sqrt{(x^2y-xy)}##
##\frac d{dt}f(x(t))=\frac d{dx}f.\frac d{dt}x##.
 
  • #25
x is a function?

x = x(t) ?
 
  • #26
EpselonZero said:
x is a function?

x = x(t) ?
Yes. In your problem x and y both depend on t, and there is a fixed relationship between x and y, so you can think of it as y depends on x depends on t.
 
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  • #27
Alright,

##f(x) = Ax^2##

##\frac{d}{dx}f = 2Ax ##
##\frac{d}{dt}x = \dot{x}^2##

##2Ax \cdot \dot{x}^2##

Is that right?
 
  • #28
EpselonZero said:
##\frac{d}{dt}x = \dot{x}^2##
Inventive.
 
  • #29
I though if ##f(x) = Ax^2, x(t) = x^2##

why not ##x^2## ?
 
  • #30
EpselonZero said:
I though if ##f(x) = Ax^2, x(t) = x^2##
What if I were to define another function g(x)=x3? Would that suddenly make x(t) equal x3?
No, x(t) just means that x is some function of t. It doesn't tell you what the function is.
##\frac{d}{dt}x=\dot x##.
 

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