Maximum Excursion (Part 2)

In the x y xy -plane, there are two massive particles. Particle 1 ( ( mass m 1 = 1 kg ) m_1 = 1\text{ kg}) is attached to a frictionless, massless wire in the shape of the curve y = α x 2 y = \alpha x^{2} , where ( α = 1 m 1 ) (\alpha = 1 \, m^{-1}) . It is free to slide along the wire, and is initially at rest at ( x , y ) = ( 1 m , 1 m ) (x,y) = (-1\text{ m},1\text{ m}) .

Particle 2 is fixed at ( x , y ) = ( 1 m , 0 m ) (x,y) = (-1\text{ m},0\text{ m}) .

There is a uniform ambient downward gravitational acceleration of 10 m/s 2 10\text{ m/s}^{2} .

Particle 1 slides down the wire under the influence of the gravitational pull of Particle 2 and of the ambient gravity. If Particle 1 reaches ( x = + 1 2 m ) \big( x = +\frac{1}{2}\text{ m}\big) before stopping and coming back, determine the mass of Particle 2 (see notes below).

Details and Assumptions:

  • The universal gravitational constant is 6.674 × 1 0 11 N m 2 / k g 2 \SI[per-mode=symbol]{6.674e-11}{\newton\meter\squared\per\kilo\gram\squared} .
  • Report your answer as the mass of Particle 2, in multiples of 1 0 11 kg 10^{11}\text{ kg} , to 2 decimal places.


The answer is 3.28.

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1 solution

Steven Chase
Nov 21, 2016

The particle stops moving at ( x , y ) = ( 1 2 , 1 4 ) (x,y) = \left(\frac{1}{2},\frac{1}{4}\right) . There are two potential energy expressions to consider. One is the interaction of the bead on the wire with the ambient field ( m 1 g y = m 1 g α x 2 ) (m_1 g y = m_1 g \alpha x^{2}) and the other is the interaction between the masses ( G m 1 m 2 r ) (\frac{-Gm_1m_2}{r}) .
The particle doesn't rise to its original height on the positive- x x side because some of the initial potential energy is going into further separating particles 1 and 2.

The potential energy balance equation is:

m 1 g ( y i y f ) = G m 1 m 2 ( 1 d i 1 d f ) m 1 g α ( 1 1 4 ) = G m 1 m 2 ( 1 1 1 ( 3 2 ) 2 + ( 1 4 ) 2 ) . \begin{aligned} m_1g(y_i - y_f) &= Gm_1m_2\left(\frac{1}{d_i} - \frac{1}{d_f}\right) \\ m_1 g \alpha\left(1 - \frac{1}{4}\right) &= Gm_1m_2 \left(\frac{1}{1} - \frac{1}{\sqrt{(\frac{3}{2})^{2} + (\frac{1}{4})^{2}}}\right). \end{aligned}

m 1 m_1 appears on both sides and cancels, allowing us to solve for m 2 m_2 . m 2 3.28 × 1 0 11 k g m_2 \approx 3.28 \times 10^{11} kg

s/charges/masses/

Shaun Griffith - 4 years, 6 months ago

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Edited, thanks

Steven Chase - 4 years, 6 months ago

hey, i did the exact same thing, just exact , but i was getting answer as 2.78 , i typed in wolfram ... 3 10/(4 6.67 (1-4/(3 sqrt5)) see it once !

A Former Brilliant Member - 4 years, 5 months ago

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