Extreme Putting

A world-class golfer wants to show off his extreme putting skills on a non-standard putting green in the shape of the following plane (distances in meters):

x y + 3 z = 0 \large{-x - y + 3z = 0}

The golfer is standing at ( x , y , z ) = ( 0 , 0 , 0 ) (x,y,z) = (0,0,0) (with the golf ball at the same location), and the hole is positioned at ( x , y , z ) = ( 10 , 20 , 10 ) (x,y,z) = (10,20,10) .

Gravity is 10 m/s 2 10 \, \text{m/s}^2 in the z -z direction.

If the ball enters the hole 10 10 seconds after being hit by the golfer, what is the ball's initial speed (in m/s \text{m/s} )?

Details and Assumptions:
- The ball can be modeled as a massive point-particle
- The ball stays on the green the entire time, and moves without losses
- The ball's initial velocity is parallel to the green
- In order to enter the hole, the ball must simply intersect the hole's coordinates


The answer is 23.6758.

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1 solution

Steven Chase
Jan 26, 2018

Here is a high-level outline of the solution. The decompositions described are performed using linear algebra.

Determine normal and tangential unit vectors to the plane (all orthogonal to each other) :

Normal: N First Tangential: t 1 Second Tangential: t 2 \text{Normal:} \, \vec{N} \\ \text{First Tangential:} \, \vec{t_1} \\ \text{Second Tangential:} \, \vec{t_2}

Represent the gravity as a superposition of these vectors (solve for component accelerations)

g = a N N + a 1 t 1 + a 2 t 2 \vec{g} = a_N \, \vec{N} + a_1 \, \vec{t_1} + a_2 \, \vec{t_2}

Planar acceleration (this is now effectively a 2D problem)

a = a 1 t 1 + a 2 t 2 \vec{a} = a_1 \, \vec{t_1} + a_2 \, \vec{t_2}

Represent the hole (xf,yf,zf) coordinates in terms of the new system coordinates (with axes aligned with the tangent vectors)

( x f , y f , z f ) ( c 1 , c 2 ) (x_f,y_f,z_f) \rightarrow (c_1,c_2)

Kinematic Equations (final time t f t_f is known; v 1 v_1 and v 2 v_2 are initial component velocities):

c 1 = v 1 t f + 1 2 a 1 t f 2 c 2 = v 2 t f + 1 2 a 2 t f 2 c_1 = v_1 \, t_f + \frac{1}{2} a_1 \, t_f^2 \\ c_2 = v_2 \, t_f + \frac{1}{2} a_2 \, t_f^2

Solve for the two component velocities (just basic algebra) and take their Euclidean norm.

I cannot figure out why my answer is wrong. I created a right triangle with a base of 1 0 2 + 2 0 2 = 10 5 \sqrt{10^2+20^2}=10\sqrt{5} and a height of 10 10 . The angle of inclination is given by θ = tan 1 1 5 \theta=\tan^{-1}{\frac{1}{\sqrt{5}}} . The acceleration along the incline is then g sin θ = g sin tan 1 1 5 = 10 6 g\sin{\theta}=g\sin{\tan^{-1}{\frac{1}{\sqrt{5}}}}=\frac{10}{\sqrt{6}} . So, the (signed) distance traveled along the incline is given by D = v t 1 2 g sin θ t 2 = v t 5 6 t 2 D=vt-\frac{1}{2}g\sin{\theta}t^2=vt-\frac{5}{\sqrt{6}}t^2 . Since the distance traveled after 10 10 seconds must be the hypotenuse of the triangle, I get 10 6 = 10 v 500 6 10\sqrt{6}=10v-\frac{500}{\sqrt{6}} , which leads to v = 6 + 50 6 v=\sqrt{6}+\frac{50}{\sqrt{6}} . But this answer differs from yours.

James Wilson - 3 years, 3 months ago

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Greetings. Regarding dimensionality, the problem starts out 3D, and can be reduced to 2D. It can't be reduced to 1D, because the physics take place on a planar region. Essentially, your solution assumes that the particle position can be described using a single direction vector, when it actually requires two direction vectors and two spatial coordinates (which I have called c1 and c2).

Steven Chase - 3 years, 3 months ago

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Oh, I understand now. Thanks so much!

James Wilson - 3 years, 3 months ago

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@James Wilson No prob, thanks for your interest in the problem

Steven Chase - 3 years, 3 months ago

If you golf, and are hitting an uphill putt on a tilted green, you can't just hit it directly toward the hole. You have to hit it a little uphill of the hole, so it rolls back toward the hole as it moves toward it.

Great problem!

G Silb - 8 months, 2 weeks ago

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