Two solid cylinders

A solid cylinder of radius R R rests on another identical cylinder that rests on the floor in an unstable equilibrium.

If the system is slightly disrupted and there's no sliding between any surfaces, with the cylinders maintaining contact, the angle θ \theta that the line joining the centers make with the vertical satisfies θ ˙ 2 = a g ( 1 cos θ ) R ( b + c cos θ d cos 2 θ ) , \dot{\theta}^2=\frac{ag(1-\cos\theta)}{R\big(b+c\cos\theta-d\cos^2\theta\big)}, where g g is the acceleration due to gravity and a , b , c , d a, b, c, d are positive integers such that the fraction is irreducible.

What is a + b + c + d ? a+b+c+d?


The answer is 37.

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2 solutions

Mark Hennings
Oct 5, 2018

I found it easier to determine the rolling conditions when I changed the sign of φ \varphi , so I have redrawn the diagram to suit. The position vector of the centre of mass G G of the bottom cylinder is O G = ( R φ R ) \overrightarrow{OG} \; = \; \left(\begin{array}{c} R\varphi \\ R \end{array}\right) The position vector of the centre of mass H H of the top cylinder is O H = ( R φ + 2 R sin θ R + 2 R cos θ ) \overrightarrow{OH} \; = \; \left(\begin{array}{c} R\varphi + 2R\sin\theta \\ R + 2R\cos\theta \end{array} \right) (this ensures that there is no slipping) which means that the two centres of mass have velocities v G = ( R φ ˙ 0 ) v H = ( R φ ˙ + 2 R cos θ θ ˙ 2 R sin θ θ ˙ ) \mathbf{v}_G \; = \; \left(\begin{array}{c} R\dot{\varphi} \\ 0 \end{array} \right) \hspace{2cm} \mathbf{v}_H \; = \; \left(\begin{array}{c} R\dot{\varphi} + 2R\cos\theta\dot{\theta} \\ -2R\sin\theta\dot{\theta} \end{array} \right) In addition, the bottom and top cylinders have angular velocities φ ˙ \dot{\varphi} and 2 θ ˙ φ ˙ 2\dot{\theta} - \dot{\varphi} respectively. Thus the kinetic energy of the system is T = 1 2 M ( R φ ˙ ) 2 + 1 4 M R 2 φ ˙ 2 + 1 2 M R 2 [ ( φ ˙ + 2 cos θ θ ˙ ) 2 + 4 sin 2 θ θ ˙ 2 ] + 1 4 M R 2 ( 2 θ ˙ φ ˙ ) 2 = 1 2 M R 2 [ 3 φ ˙ 2 + 6 θ ˙ 2 + 2 ( 2 cos θ 1 ) φ ˙ θ ˙ ] \begin{aligned} T & = \; \tfrac12M(R\dot{\varphi})^2 + \tfrac14MR^2\dot{\varphi}^2 + \tfrac12MR^2\big[(\dot{\varphi} + 2\cos\theta\dot{\theta})^2 + 4\sin^2\theta\dot{\theta}^2\big] + \tfrac14MR^2(2\dot{\theta}-\dot{\varphi})^2 \\ & = \; \tfrac12MR^2\big[3\dot{\varphi}^2 + 6\dot{\theta}^2 + 2(2\cos\theta-1)\dot{\varphi}\dot{\theta}\big] \end{aligned} and so the Lagrangian of the system is L = T 2 M g R cos θ \mathcal{L} = T - 2MgR\cos\theta . Since L \mathcal{L} is independent of φ \varphi , it follows that L φ ˙ \frac{\partial \mathcal{L}}{\partial \dot{\varphi}} is a constant of the motion, and hence we deduce that 3 φ ˙ + 2 ( 2 cos θ 1 ) θ ˙ = 0 3\dot{\varphi} + 2(2\cos\theta-1)\dot{\theta} \; = \; 0 Conservation of energy now tells us that 1 2 M R 2 [ 3 φ ˙ 2 + 6 θ ˙ 2 + 2 ( 2 cos θ 1 ) φ ˙ θ ˙ ] + 2 M g R cos θ = 2 M g R \tfrac12MR^2\big[3\dot{\varphi}^2 + 6\dot{\theta}^2 + 2(2\cos\theta-1)\dot{\varphi}\dot{\theta}\big] + 2MgR\cos\theta \; = \; 2MgR Substituting φ ˙ = 2 3 ( 2 cos θ 1 ) θ ˙ \dot{\varphi} = -\tfrac23(2\cos\theta-1)\dot{\theta} into this equation yields the formula θ ˙ 2 = 12 g ( 1 cos θ ) R ( 17 + 4 cos θ 4 cos 2 θ ) \dot{\theta}^2 \; = \; \frac{12g(1-\cos\theta)}{R(17 + 4\cos\theta - 4\cos^2\theta)} making the answer 12 + 17 + 4 + 4 = 37 12 + 17 + 4 + 4 = \boxed{37} .

How were we supposed to know whether the part of the cylinder touching the floor was the rounded part of the cylinder or the flat part of the cylinder?

Kermit Rose - 2 years, 5 months ago

What is θ with dot on top of it?

Hunt Ethan - 1 year, 4 months ago

The derivative of θ \theta with respect to time - this is a very common convention in mechanics.

Mark Hennings - 1 year, 4 months ago

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Oh now i get it, i learnt that as using the symbol 'small omega' for angular velocity. If you don't mind can you also tell what is this used for φ? And this phi with dot on top as well. And i haven't seen the vector denotion you used by using () so i would appreciate if you can explain that also. Thanks :)

PS: i didn't expect this thing was still active :p

Hunt Ethan - 1 year, 4 months ago
Vinod Kumar
Oct 15, 2018

Cylinder rolling on another cylinder is well known problem and the numbers in the expression sum to:

Answer=12+17+4+4=37

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