2023 A/L Physics Past Paper · Question 41 (English Medium)

Acceleration of the upper block just after the string breaks

Two identical blocks AA and BB connected by a light spring are suspended by a string attached to the ceiling as shown in the figure. Initially the system is at rest and then suddenly the string breaks. Immediately after the string is broken, what will be the downward acceleration of the upper block AA?

  1. (1) 00
  2. (2) g2\dfrac{g}{2}
  3. (3) gg
  4. (4) 2 g\sqrt{2}\,g
  5. (5) 2g2g
Answer and explanation

Answer: (5) 2g2g

What the question asks

We want: the downward acceleration aAa_A of the upper block, just after the string breaks.

What each letter means:

mm (kg\text{kg}): the mass of each block. The two blocks are identical.

gg (m s−2\text{m s}^{-2}): the acceleration of gravity.

FsF_s (N\text{N}): the force of the spring.

aAa_A (m s−2\text{m s}^{-2}): the downward acceleration of the block AA, just after the string breaks.

Relevant theory

Newton's first law states that a resultant force can change the state of motion of an object. Newton's second law states about this resultant force.

where k is the constant of proportionality and is called the force constant of the wire. The

The first quote gives Newton's second law, F=maF = ma: the resultant force on a body gives it an acceleration. The second quote says that the force of a stretched wire or spring grows with its extension, F=keF = ke.

For example, hold a stretched elastic band with a bag hanging at its lower end. The band pulls the bag up and pulls your hand down with the same force.

Let go of your hand. The band cannot shrink in an instant, so for that instant it still pulls the same.

Required equations

Fs=mgF_s = mg

mg+Fs=maAmg + F_s = m a_A

mg+mg=maAmg + mg = m a_A

aA=2ga_A = 2g

Reasoning and calculation

Before the string breaks:

The block BB hangs at rest. Two forces act on it: its weight mgmg down, and the pull of the spring FsF_s up. They balance, so Fs=mgF_s = mg.

The spring pulls BB up. It pulls AA down with the same force, mgmg.

mgmg

Fs=mgF_s = mg

Just after the string breaks:

The string pull on AA is gone. The spring has not had time to change its length, so it still pulls with Fs=mgF_s = mg.

Now the block AA has two forces, both downward: its weight mgmg and the spring pull mgmg. Newton's second law gives mg+mg=maAmg + mg = m a_A.

2mg=maA2mg = m a_A

mg+mg=maAmg + mg = m a_A

2g2g

aA=2mgma_A = \dfrac{2mg}{m}

1010

Fs=1×10F_s = 1 \times 10

2020

mg+Fs=10+10mg + F_s = 10 + 10

aA=201a_A = \dfrac{20}{1}

(m∗g+m∗g)/m(m * g + m * g) / m

Reading the options

Now compare 2g2g with the five options.

Option (5) is 2g2g. It matches.

Option (1) is zero, option (2) is g2\dfrac{g}{2}, option (3) is gg and option (4) is 2 g\sqrt{2}\,g. None of these is 2g2g.

Checks

Check the units. In mg+Fs=maAmg + F_s = m a_A, each term is a force, in N\text{N}. Divide by mm and each term is an acceleration, in m s−2\text{m s}^{-2}.

So aA=2ga_A = 2g is in m s−2\text{m s}^{-2}, as an acceleration must be.

Does it make sense?

Think of the block BB. Just after the break the spring pulls it up with mgmg and its weight pulls it down with mgmg. They balance, so BB has no acceleration for that instant.

If the spring were not there, the block AA would fall with gg. The spring pull adds one more gg, so 2g2g is a fair size.

Conclusion

aA=2ga_A = 2g

Just after the string breaks, the downward acceleration of the block AA is 2g2g.

The answer is (5).

The quotes give Newton's second law and the force of a stretched spring. The steps that the spring keeps its pull at the instant the string breaks, and that the block BB is at rest before it, are our reasoning from them.

Teacher's note

Draw the forces on the block you want, just after the change. The spring keeps its pull for that instant. Add the forces on the one line, then use F=maF = ma.

Exam tip

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