Circular Motion: Particle on a String

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Homework Help Overview

The problem involves a particle of mass hanging from a string, which is given an initial horizontal velocity and is expected to complete a vertical circular motion. The context is circular motion and energy conservation principles.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between the initial speed and the speed at the top of the circle, questioning the assumptions about constant velocity. They explore the application of conservation of mechanical energy to relate energies at different points in the motion.

Discussion Status

Some participants have provided guidance on the application of conservation laws and clarified the relationship between forces acting on the particle at different points in the circular path. There is an acknowledgment of the need for further calculations regarding momentum after a collision with another particle.

Contextual Notes

Participants note the requirement for the string to remain taut at the highest point of the circle and the implications of the initial conditions set by the problem statement. There is also mention of a second part of the question involving a collision, which introduces additional complexity to the analysis.

rock.freak667
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Homework Statement



A particle,A, of mass,m, hangs by a light inextensible string of length,a from a fixed point O. The string is initially vertical and the particle is then given a horizontal velocity,[itex]\sqrt{nga}[/itex]. Show that it will move round a complete vertical circle in a vertical plane provided [itex]n \geq 5[/itex]


Homework Equations



Centripetal force=[itex]\frac{mv^2}{r}[/itex]


The Attempt at a Solution



Well the resultant force of the tension in the string and the component of the weight provides the centripetal force.

[itex]F_c=T-W_{component}[/itex]

[tex]\frac{mv^2}{a}=T-mgcos\alpha...(*)[/tex]

If initially it is vertical then [itex]\alpha=0[/itex] (Doesn't really seem to help)

For the object to make a complete circle, then the string must be taut at the highest point (i.e. when [itex]\alpha=180,T\geq 0[/itex]

From (*)
[tex]T=\frac{mv^2}{a}+mgcos180 \Rightarrow T=\frac{m(\sqrt{nga})^2}{a}-mg[/tex]

So that

T=mgn-mg

For [itex]T \geq 0[/itex] then [itex]mng \geq mg \Rightarrow n \geq 1[/itex]

Which is not what I want to show.
 
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Two points:
(1) At the top, the centripetal acceleration and the weight both point downward and thus have the same sign.
(2) [itex]\sqrt{nga}[/itex] is the initial speed at the bottom of the circle, not the speed at the top. How are those speeds related?
 
Doc Al said:
Two points:
(1) At the top, the centripetal acceleration and the weight both point downward and thus have the same sign.
At the top the tension and weight point downwards and that provides the centripetal force..I hope
Doc Al;1713800(2) [itex said:
\sqrt{nga}[/itex] is the initial speed at the bottom of the circle, not the speed at the top. How are those speeds related?

oh..they aren't the same. I thought they were, I read given a horizontal velocity to mean that it moves with that velocity throughout the motion.

Well by the law of conservation of mechanical energy, (relative to the horizontal line through O)

Energy at the bottom=Energy at the top
[tex]\frac{1}{2}m(\sqrt{nga})^2-mga=\frac{1}{2}mV^2+mga[/tex]

and so

[tex]mV^2= mgan-4mga[/tex]

and putting that into the eq'n with tension

[tex]T=\frac{mgan-4mga}{a}-mg[/tex]
[tex]\Rightarrow T=mgn-5mg=mg(n-5)[/tex]
and [itex]m\neq 0,g\neq[/itex], the only way for [itex]T\geq0[/itex] is if [itex]n \geq 5[/itex]

Thanks for that!
 
I forgot to put in the 2nd part of the question.

"If when the string OA reaches the horizontal, the particle A collides and coalesces with a second particle at rest also of mass m, find the least value of n for the vertical circle to be completed."

I think I must use the law of conservation of momentum here.

To get the velocity at A, use law of conservation of M.E.


[tex]\frac{1}{2}mnga-mga=\frac{1}{2}mV_{a}^2[/tex]

[tex]V_a=\sqrt{nga-2ga}[/tex]

Initial momentum = [itex]mV_a[/itex]
= [itex]m\sqrt{nga-2ga}[/itex]

Final momentum = [itex]2mV_f[/itex]

By the law of conservation of momentum.

[tex]2mV_f=m\sqrt{nga-2ga}[/tex]

[tex]V_f=\sqrt{nga-2ga}[/tex]

Correct so far?
 
rock.freak667 said:
[tex]2mV_f=m\sqrt{nga-2ga}[/tex]

[tex]V_f=\sqrt{nga-2ga}[/tex]
All good except for that last step--you left off the factor of 2 in the denominator.
 

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