3D Pendulum (Part 2)

A point mass m = 1 m = 1 is attached to the free end of a mass-less rigid rod of length L = 1 L = 1 . The other end of the rod is attached to the origin with a ball joint, allowing the free end to be positioned at an arbitrary point in 3 D 3D space (constrained by the length of the rod, or course). The gravitational acceleration is 10 10 in the negative z z direction.

If the rod rotates in such a way that its free end is constantly at z = 0.5 z = -0.5 , what is the linear speed of the free end?


The answer is 3.873.

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3 solutions

Karan Chatrath
Apr 30, 2020

Pendulum parameterised in spherical coordinates:

x = sin θ cos ϕ x = \sin{\theta} \cos{\phi} y = sin θ sin ϕ y = \sin{\theta} \sin{\phi} z = cos θ z = \cos{\theta}

The equations of motion were derived in the previous version of this problem. They read:

θ ¨ = ϕ ˙ 2 sin θ cos θ + 10 sin θ \ddot{\theta} = \dot{\phi}^2 \ \sin{\theta} \cos{\theta} + 10\sin{\theta} ϕ ¨ = 2 θ ˙ ϕ ˙ cot θ \ddot{\phi} = -2 \dot{\theta} \ \dot{\phi} \cot{\theta}

It is given that z = 0.5 z= -0.5 .

θ = arccos ( 0.5 ) = 2 π 3 \implies \theta = \arccos(-0.5) = \frac{2\pi}{3}

This implies that θ \theta is always constant and its higher derivatives are always zero. Using this fact in the equations of motion:

ϕ ¨ = 0 θ ˙ = 0 \ddot{\phi} = 0 \ \because \dot{\theta}=0 θ ¨ = 0 ϕ ˙ 2 = 10 cos θ ϕ ˙ 2 = 20 \ddot{\theta}=0 \ \implies \dot{\phi}^2 = \frac{-10}{\cos{\theta}} \implies \dot{\phi}^2 = 20

Finally taking the time derivatives of the coordinates of the pendulum gives:

x ˙ = sin θ sin ϕ ϕ ˙ \dot{x} = -\sin{\theta} \sin{\phi} \ \dot{\phi} y ˙ = sin θ cos ϕ ϕ ˙ \dot{y} = \sin{\theta} \cos{\phi} \ \dot{\phi} z ˙ = 0 θ ( t ) = 2 π 3 \dot{z} = 0 \ \because \theta(t) = \frac{2\pi}{3}

FInally, the speed is:

V = x ˙ 2 + y ˙ 2 = sin θ ϕ ˙ = 3 2 20 = 3 × 20 4 = 15 V = \sqrt{\dot{x}^2 + \dot{y}^2} = \sin{\theta}\dot{\phi} = \frac{\sqrt{3}}{2}\sqrt{20} = \sqrt{\frac{3 \times 20}{4}} = \sqrt{15}

Answer is:

V = 15 \boxed{V = \sqrt{15}}

@Karan Chatrath How to solve that 2nd order equation??

A Former Brilliant Member - 1 year, 1 month ago
Amal Hari
May 1, 2020

Taking the assumption that it is constrained at x = 0.5 x=-0.5 , we can infer three things:

(1) vertical force is 0

(2) Horizontal force is m v 2 r \frac{mv^{2}}{r}

(3) The angle subtended by the rod with z axis is 60 degrees

Based on these, we can draw a F.B.D and get the following equations by letting F F , the force exerted by the rod on point mass:

(1) F sin ( 30 ) = m g F\sin (30) =mg

F = 20 F=20

(2) F cos ( 30 ) = m v 2 r F\cos (30)= \frac{mv^{2}}{r}

10 3 = 1 × v 2 1 × cos ( 30 ) 10\sqrt{3}=\frac{1\times v^{2}}{1\times \cos(30)}

15 = v 2 15=v^{2}

v = 15 v=\sqrt{15}

v 3.873 v\approx 3.873

This problem actually describes a conical pendulum . Let the rod subtends an angle of α α with vertical. Then the linear velocity v v is related to the angular velocity ω \omega through v = ω sin α v=\omega \sin α . Now, cos α = 0.5 = g ω 2 \cos α=0.5=\dfrac{g}{\omega^2} . So ω = 2 g v = ω sin α = 2 g × 3 2 = 3 g 2 = 15 3.873 \omega=\sqrt {2g}\implies v=\omega\sin α=\sqrt {2g}\times \dfrac{\sqrt 3}{2}=\sqrt {\frac{3g}{2}}=\sqrt {15}\approx \boxed {3.873} .

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