2021 A/L Physics Past Paper · Question 18 (English Medium)

Tensions on the two sides of a pulley that turns

A block placed on a horizontal frictionless table is attached to mass mm by a light inextensible string that passes over a pulley as shown in the figure. When released from rest, mass mm and the pulley accelerate. If the tensions in the sections in the string are T1T_1 and T2T_2 as marked, which of the following is true?

  1. (1) mg=T1=T2mg = T_1 = T_2
  2. (2) mg>T1=T2mg > T_1 = T_2
  3. (3) mg>T1<T2mg > T_1 < T_2
  4. (4) mg=T1>T2mg = T_1 > T_2
  5. (5) mg>T1>T2mg > T_1 > T_2
Answer and explanation

Answer: (5) mg>T1>T2mg > T_1 > T_2

Given information

We know:

The block has mass MM. The table is frictionless.

The string is light and inextensible. It moves with the block, round the rim of the pulley, and with mm.

The pulley has a moment of inertia II and radius rr. It turns as the string moves.

What the question asks

We want to compare mgmg, T1T_1 and T2T_2.

The string cannot stretch. So the block, the mass mm and the rim of the pulley all move together.

They share one acceleration aa, and a=rαa = r\alpha for the rim.

Relevant theory

According to Newton's second law resultant force is proportional to the rate of change of momentum.

In translatory motion, force is defined as the rate of change of linear momentum. Likewise in rotational motion, torque or moment of the force is defined as the rate of change of angular momentum.

Required equations

a=rαa = r\alpha

T2=MaT_2 = Ma

mg−T1=mamg - T_1 = ma

(T1−T2) r=Iα(T_1 - T_2)\,r = I\alpha

Applying it to this question

Apply the law to each body.

The block: only T2T_2 pulls it along the table. So T2=MaT_2 = Ma.

The mass mm: the weight mgmg pulls down and T1T_1 pulls up. So mg−T1=mamg - T_1 = ma.

The pulley: T1T_1 turns it one way and T2T_2 turns it back. So (T1−T2) r=Iα(T_1 - T_2)\,r = I\alpha.

mg=(M+m+Ir2)amg = \left(M + m + \dfrac{I}{r^2}\right)a

22

a=1×102+1+0.5/0.25=2a = \dfrac{1 \times 10}{2 + 1 + 0.5/0.25} = 2

44

T2=Ma=2×2=4T_2 = Ma = 2 \times 2 = 4

88

T1=m(g−a)=1×(10−2)=8T_1 = m(g - a) = 1 \times (10 - 2) = 8

Reasoning and calculation

Signs first. Take the way each body moves as positive.

The block moves toward the pulley, the mass mm moves down, and the pulley turns the way T1T_1 pulls it.

Then T2T_2 pulls the block forward, T1T_1 pulls the pulley forward, and T2T_2 holds the pulley back.

Put α=ar\alpha = \dfrac{a}{r} in the pulley equation:

T1−T2=Iar2T_1 - T_2 = \dfrac{I a}{r^2}

The pulley accelerates, so a>0a > 0. Then T1−T2>0T_1 - T_2 > 0, and T1>T2T_1 > T_2.

From the hanging mass:

mg−T1=ma>0mg - T_1 = ma > 0

So mg>T1mg > T_1.

Together: mg>T1>T2mg > T_1 > T_2. Option (5).

Checks

Limiting case. If the pulley had no moment of inertia, I→0I \to 0.

Then T1−T2=0T_1 - T_2 = 0 and T1=T2T_1 = T_2. This is option (2), the usual light pulley.

The question says the pulley accelerates, so II is not zero, and T1>T2T_1 > T_2.

m∗g/(M+m+I/(r∗r))m * g / (M + m + I / (r * r))

Conclusion

mg>T1>T2mg > T_1 > T_2

The pulley turns faster, so T1>T2T_1 > T_2. The mass mm accelerates down, so mg>T1mg > T_1.

The answer is (5).

A pulley with a moment of inertia needs a net torque to turn faster.

So the two tensions on its sides are not equal. The side that pulls the pulley round has the larger tension.

Exam tip

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