2024 A/L Physics Past Paper · Question 16 (English Medium)

Two boxes pushed together

Two boxes AA and BB of mass 10 kg10\ \text{kg} and 5 kg5\ \text{kg} respectively and made of different materials are placed on a rough horizontal surface as shown in the figure. The coefficient of kinetic friction between box AA and the surface is 0⋅50{\cdot}5. When a horizontal force of 100 N100\ \text{N} is applied to box AA, the reaction force between boxes AA and BB is 40 N40\ \text{N}. What would be the coefficient of kinetic friction between box BB and the horizontal surface?

  1. (1) 0⋅70{\cdot}7
  2. (2) 0⋅60{\cdot}6
  3. (3) 0⋅50{\cdot}5
  4. (4) 0⋅40{\cdot}4
  5. (5) 0⋅30{\cdot}3
Answer and explanation

Answer: (1) 0⋅70{\cdot}7

Given information

This question is about pushing two boxes that touch, along a rough floor.

A force of 100 N100\ \text{N} pushes box AA. Box AA pushes box BB in front of it, so both slide together.

The boxes are made of different materials, so the floor rubs on each one differently. We know the friction for AA. We also know that AA and BB push on each other with 40 N40\ \text{N}.

What we must find: the coefficient of kinetic friction between box BB and the floor.

How we find it: use AA alone to find the acceleration they share. Then use BB alone to find its friction.

mA=10 kgm_A=10\ \text{kg} and mB=5 kgm_B=5\ \text{kg}. The push on AA is F=100 NF=100\ \text{N}. For AA, μA=0.5\mu_A=0.5. The force between the boxes is P=40 NP=40\ \text{N}. Take g=10 m s−2g=10\ \text{m s}^{-2}.

What the question asks

mAm_A, mBm_B (kg\text{kg}): masses of AA and BB.

FF (N\text{N}): horizontal force on AA.

PP (N\text{N}): reaction force between AA and BB.

RAR_A, RBR_B (N\text{N}): normal contact forces from the floor.

FAF_A, FBF_B (N\text{N}): kinetic friction forces on AA and BB.

μA\mu_A, μB\mu_B: coefficients of kinetic friction.

aa (m s−2\text{m s}^{-2}): acceleration of both boxes.

Relevant theory

∴F=ma\therefore F = ma

F - Resultant force in newtons m - mass in kg a - acceleration in m s^-2

The dynamic friction acting on an object is also proportional to the normal contact force between surfaces. If the dynamic friction is FdF_d and normal contact force is R,

Fd∝RF_d \propto R Fd=μdRF_d = \mu_d R

μd\mu_d is called the coefficient of dynamic friction.

When the objects interact (collide), they exert equal and oppsite forces on one another.

What is happening: the boxes stay in contact, so they speed up together with the same aa.

Box AA is pushed forward by 100 N100\ \text{N}. It is held back by its friction and by BB, which pushes back on it with 40 N40\ \text{N}.

Box BB is pushed forward only by AA, with the same 40 N40\ \text{N}. It is held back only by its own friction.

The floor is horizontal, so each normal contact force equals the weight: R=mgR=mg.

For example, push two school desks in a line. You push only the back desk.

The back desk pushes the front desk. That push is the only thing moving the front desk forward.

If the front desk drags hard on the floor, it needs a bigger push to keep up.

In words: look at each desk on its own. The push between them tells us how hard the floor drags on the front one.

Required equations

FA=μARA=μAmAgF_A=\mu_AR_A=\mu_Am_Ag

F−FA−P=mAaF-F_A-P=m_Aa

P−μBmBg=mBaP-\mu_Bm_Bg=m_Ba

Applying it to this question

100100

RA=10×10R_A=10\times10

5050

FA=0.5×100F_A=0.5\times100

100−50−40=10a100-50-40=10a

10=10a10=10a

11

aa

40−FB=5×140-F_B=5\times1

3535

FBF_B

RB=5×10R_B=5\times10

μB=3550\mu_B=\dfrac{35}{50}

0.70.7

μB\mu_B

Reasoning and calculation

Both boxes must have a=1 m s−2a=1\ \text{m s}^{-2}. Only μB=0.7\mu_B=0.7 leaves BB with exactly 40−35=5 N40-35=5\ \text{N} to give its 5 kg5\ \text{kg} that acceleration. This is option (1).

With 0.60.6, the friction on BB is 30 N30\ \text{N}. Then BB would have a=(40−30)/5=2 m s−2a=(40-30)/5=2\ \text{m s}^{-2}. But AA has a=1 m s−2a=1\ \text{m s}^{-2}, and the boxes move together.

0.50.5 copies the coefficient of AA. The boxes are made of different materials, so there is no reason for the same value. With 0.50.5, BB would have a=(40−25)/5=3 m s−2a=(40-25)/5=3\ \text{m s}^{-2}, not 1 m s−21\ \text{m s}^{-2}.

0.40.4 comes from 40/10040/100, the push between the boxes divided by the applied force. Friction coefficient is friction divided by RR. With 0.40.4, BB would have a=(40−20)/5=4 m s−2a=(40-20)/5=4\ \text{m s}^{-2}.

With 0.30.3, the friction on BB is only 15 N15\ \text{N}. Then BB would have a=(40−15)/5=5 m s−2a=(40-15)/5=5\ \text{m s}^{-2}, five times the acceleration of AA. BB would run away from AA, but the 40 N40\ \text{N} push says they stay in contact.

Checks

(40−5∗1)/(5∗10)(40-5*1)/(5*10)

F−FA−FB=(mA+mB)aF-F_A-F_B=(m_A+m_B)a

100−50−35=15×1100-50-35=15\times1

15 N=15 N15\ \text{N}=15\ \text{N}

μB=FB/RB\mu_B=F_B/R_B is N\text{N} divided by N\text{N}, so it has no unit, as a friction coefficient should.

Taken together, the inside pushes of 40 N40\ \text{N} cancel, and the check works without them. The friction on BB, 35 N35\ \text{N}, is less than the 40 N40\ \text{N} push it gets, so BB speeds up forwards, as it should.

Conclusion

μB=0.7\mu_B=0.7

The coefficient of kinetic friction for BB is 0.70.7. The answer is (1).

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