Circular Motion: Particle on a String

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A particle of mass m hangs from a string of length a and is given an initial horizontal velocity of √(nga). For the particle to complete a vertical circle, the tension in the string must be non-negative at the highest point, leading to the condition n ≥ 5. The discussion highlights the importance of distinguishing between the initial speed at the bottom of the circle and the speed at the top, which is derived from conservation of energy. Additionally, when the particle collides with a second mass at rest, conservation of momentum is applied to find the new conditions for completing the circle. The calculations confirm that the least value of n for the vertical circle to be completed remains critical for both scenarios.
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,\sqrt{nga}. Show that it will move round a complete vertical circle in a vertical plane provided n \geq 5


Homework Equations



Centripetal force=\frac{mv^2}{r}


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.

F_c=T-W_{component}

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

If initially it is vertical then \alpha=0 (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 \alpha=180,T\geq 0

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

So that

T=mgn-mg

For T \geq 0 then mng \geq mg \Rightarrow n \geq 1

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) \sqrt{nga} 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
\frac{1}{2}m(\sqrt{nga})^2-mga=\frac{1}{2}mV^2+mga

and so

mV^2= mgan-4mga

and putting that into the eq'n with tension

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

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.


\frac{1}{2}mnga-mga=\frac{1}{2}mV_{a}^2

V_a=\sqrt{nga-2ga}

Initial momentum = mV_a
= m\sqrt{nga-2ga}

Final momentum = 2mV_f

By the law of conservation of momentum.

2mV_f=m\sqrt{nga-2ga}

V_f=\sqrt{nga-2ga}

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

V_f=\sqrt{nga-2ga}
All good except for that last step--you left off the factor of 2 in the denominator.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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