Day 2: Let It Snow!

It's a snow day, and Tommy has decided to go sledding on the tobogganing hill down near the lake. Tommy estimates the hill is 20 20 metres tall, and is positioned facing the lake (at this time of year, the lake is completely frozen). Tommy decides to roll a large snowball and place it across the lake, and order to stop his toboggan once he has reached the bottom of the hill, and has slid across the lake. When Tommy collides with the snowball, they will travel as one combined mass forward. If Tommy estimates snowball to be 20 20 kilograms, and his combined mass with the sled to be 55 55 kilograms, how far (in metres) will he and the snowball slide before coming to a complete stop?

Details and Assumptions

The efficiency of the energy exchange between Tommy's energy at the top of the hill, and the bottom of the hill is 30 30 %

The coefficient of friction between Tommy and the frozen pond is negligible.

The coefficient of friction between the combined Tommy-snowball mass and the snow is 0.38 0.38 .

Take gravity to be 9.81 m/s 2 9.81 \ \text{m/s}^2 .

Round all values obtained while solving this problem to three significant digits.


This problem is part of The 12 Days of Math-Mas 2018


The answer is 8.41.

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2 solutions

Steven Chase
Dec 3, 2018

Glossary: Hill height = H Snow mass = m Tommy mass = M Hill conversion efficiency = ϵ Snow friction coefficient = μ Gravity acceleration = g \text{Hill height} = H \\ \text{Snow mass} = m \\ \text{Tommy mass} = M \\ \text{Hill conversion efficiency} = \epsilon \\ \text{Snow friction coefficient} = \mu \\ \text{Gravity acceleration} = g \\

Compute these steps sequentially to get the final answer:

Change in gravitational potential energy: Δ U = M g H \Delta U = M g H

Kinetic energy at hill bottom: E b = ϵ Δ U E_b = \epsilon \, \Delta U

Speed at bottom: v b = 2 E b M v_b = \sqrt{\frac{2 E_b}{M}}

Momentum conservation upon collision with snowball: M v b = ( M + m ) v f v f = M v b M + m M \, v_b = (M + m) \, v_f \\ v_f = \frac{M \, v_b}{M + m}

Kinetic energy of combined mass after collision: E f = 1 2 ( M + m ) v f 2 E_f = \frac{1}{2} (M + m) \, v_f^2

Friction force on combined mass: F = μ ( M + m ) g F = \mu \, (M + m) \, g

Distance slid over snow: E f = F D D = E f F E_f = F \, D \\ D = \frac{E_f}{F}

Computing all of this results in D 8.49 D \approx 8.49

Jack Ceroni
Dec 17, 2018

We know that Tommy's energy at the top of the hill is E i = m g h = ( 55 ) ( 9.81 ) ( 20 ) = 10791 E_i \ = \ mgh \ = \ (55)(9.81)(20) \ = \ 10791 . We know that all of the gravitational potential energy will be converted to kinetic energy, with 30 30 % efficiency, so the energy at the bottom of the hill will be ( E i ) ( P E ) = ( 10791 ) ( 0.3 ) = 3237.3 (E_i)(PE) \ = \ (10791)(0.3) \ = \ 3237.3 . Solving for the velocity, we get E k = 1 2 m v 2 = 3237.3 v = 10.8 m / s E_k \ = \ \frac{1}{2}mv^2 \ = \ 3237.3 \ \Rightarrow \ v \ = \ 10.8 \ m/s . Tommy will then slide across the lake at the same velocity and collide with the snowball. Because of conservation of momentum, we get Σ p i = Σ p f ( 55 ) ( 10.8 ) = ( 75 ) v i \Sigma \ p_i \ = \ \Sigma \ p_f \ \Rightarrow \ (55)(10.8) \ = \ (75)v_i . So the initial velocity of the combine mass is v i = 7.92 m / s v_i \ = \ 7.92 \ m/s . We can solve for the acceleration of the combined mass by noting the only unbalanced force acting on the combined mass is friction, which will act in the opposite direction of motion with magnitude F f = m g μ k = ( 75 ) ( 9.81 ) ( 0.38 ) = 280 N F_f \ = \ mg\mu_k \ = \ (75)(9.81)(0.38) \ = \ 280 \ N , so the acceleration is F f m \frac{F_f}{m} , or 3.73 m / s -3.73 \ m/s . Using the equation v f 2 = v i 2 + 2 a d v_f^{2} \ = \ v_i^{2} \ + \ 2ad , we can solve for d d easily by noting that the final velocity will be 0 0 . We get: ( 7.92 ) 2 = 2 ( 3.73 ) ( d ) d = 8.41 -(7.92)^2 \ = \ 2(-3.73)(d) \ \Rightarrow \ d \ = \ 8.41 .

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