2021 A/L Physics Past Paper · Question 26 (English Medium)

Terminal velocity of a small drop in air

A small spherical liquid drop of radius rr and density ρ\rho falls with terminal velocity vv in still air. The coefficient of viscosity of air is η\eta and the density of air can be neglected. Consider the following statements regarding the terminal velocity vv of the droplet.

(A) It is directly proportional to r2r^2.

(B) It is directly proportional to ρ\rho.

(C) It is inversely proportional to η\eta.

Of the above statements,

  1. (1) Only (A) is true.
  2. (2) Only (B) is true.
  3. (3) Only (A) and (B) are true.
  4. (4) Only (B) and (C) are true.
  5. (5) All (A), (B) and (C) are true.
Answer and explanation

Answer: (5) All (A), (B) and (C) are true.

What the question asks

Find which of the statements (A), (B) and (C) are true.

They say how the terminal velocity vv depends on rr, ρ\rho and η\eta.

The plan: find vv in terms of rr, ρ\rho and η\eta, then test each statement.

Relevant theory

The sphere now begins to move with a uniform velocity.

This expression is referred to as Stokes’ law.

Reading the options

The options are combinations of (A), (B) and (C).

At the terminal velocity the weight equals the viscous force:

43πr3ρg=6πηrv\tfrac{4}{3}\pi r^3 \rho g = 6\pi\eta r v

So:

v=2r2ρg9ηv = \dfrac{2 r^2 \rho g}{9\eta}

We test each statement on this result.

Reasoning and calculation

It is directly proportional to r2r^2.

rr appears as r2r^2 in the top of the fraction. The other symbols stay the same. So v∝r2v \propto r^2.

A

It is directly proportional to ρ\rho.

ρ\rho is in the top of the fraction, to the power 11. So v∝ρv \propto \rho.

B

It is inversely proportional to η\eta.

η\eta is in the bottom of the fraction. So v∝1ηv \propto \dfrac{1}{\eta}.

C

All three statements follow from v=2r2ρg9ηv = \dfrac{2 r^2 \rho g}{9\eta}.

So (A), (B) and (C) are all true.

Why the other options fail

(B) and (C) are true too, so (A) alone is not enough.

(A) and (C) are true too, so (B) alone is not enough.

(C) is true too, because η\eta is in the bottom of the fraction.

(A) is true too, because v∝r2v \propto r^2.

Conclusion

v=2r2ρg9ηv = \dfrac{2 r^2 \rho g}{9\eta}.

(A), (B) and (C) are all true. The answer is (5).

At terminal velocity the forces balance. Write weight == Stokes force, solve for vv, and read off each dependence.

Look at which symbols sit on top and which sit at the bottom.

Exam tip

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