2023 A/L Physics Past Paper · Question 33 (English Medium)

Two charged droplets when the plates are brought closer

A voltage is applied across two parallel conducting plates. As shown in the figure two charged droplets XX and YY of masses 2m2m and mm respectively are at rest between the plates. Neglect the interaction between XX and YY. When two plates are brought closer,

  1. (1) XX and YY remain at equilibrium.
  2. (2) XX and YY fall down with equal accelerations.
  3. (3) XX and YY rise up with equal accelerations.
  4. (4) XX rises with greater acceleration than YY.
  5. (5) XX falls down with greater acceleration than YY.
Answer and explanation

Answer: (3) XX and YY rise up with equal accelerations.

What the question asks

What is changed: the plates are brought closer. The voltage across them stays the same, so only the distance dd between them gets smaller.

We want: what XX and YY do after that.

What each letter means:

VV (V\text{V}): the voltage across the plates.

dd (m\text{m}): the distance between the plates.

EE (V m−1\text{V m}^{-1}): the electric field intensity between the plates.

qq (C\text{C}): the charge of a droplet.

mm (kg\text{kg}): the mass of a droplet.

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

aa (m s−2\text{m s}^{-2}): the acceleration of a droplet.

Relevant theory

The electric field intensity at a certain point in an electric field is the force acting ona unit positive (+) charge placed at that point.

Hence, the force acting on a charge "q" placed at a point of intensity E is F = Eq.

Hence according to the above expression, the electric field intensity at any point in an electric field is equal to the potential gradient at that point.

The first quote says the electric field intensity at a point is the force on a unit positive charge there. The second quote gives the force on a charge qq as F=EqF = Eq. The third quote says the field intensity equals the potential gradient.

Between two parallel plates the potential changes evenly from one plate to the other, so the gradient is the voltage over the distance, E=VdE = \dfrac{V}{d}.

For example, think of two lifts hanging still at one floor, a big lift and a small one. The cable of each lift pulls up exactly as much as its weight, so the big lift has a harder pull.

Now make each cable pull a tenth more than before. For each lift the extra pull is a tenth of its weight, so both lifts speed up upwards by the same amount, however heavy they are.

Applying it to this question

qE=mgqE = mg

E=VdE = \dfrac{V}{d}

qm=gE\dfrac{q}{m} = \dfrac{g}{E}

Reasoning and calculation

What stays the same: the voltage VV (the battery is still connected), the charge qq and the mass mm of each droplet, and gg.

What changes: the distance dd gets smaller. So the field E=VdE = \dfrac{V}{d} gets bigger.

Which way is the net force?

Before: the upward force qEqE was equal to the weight mgmg.

After: EE is bigger, so the upward force qE′qE' is bigger than the weight mgmg. The net force is up, so both droplets rise.

How much faster does each one go?

The net upward force is qE′−mgqE' - mg. Divide by the mass mm.

a=qE′m−ga = \dfrac{qE'}{m} - g

Put in qm=gE\dfrac{q}{m} = \dfrac{g}{E}.

a=g(E′E−1)a = g\left(\dfrac{E'}{E} - 1\right)

The mass is not in this. It is the same for XX and YY, and it is upward, so aa is positive.

Reading the options

Now match it with the five options.

(1) They stay at rest. The net force is not zero. It does not match.

(2) They fall. The net force is up. It does not match.

(3) They rise with equal accelerations. This matches.

(4) XX rises faster than YY. The accelerations are equal. It does not match.

(5) XX falls faster than YY. It does not match.

Why the other options fail

The upward force grows when EE grows, so the droplets are no longer in balance.

The net force is up, because qE′qE' is bigger than mgmg.

The mass cancels, so XX and YY have the same acceleration.

The droplets rise, and the mass cancels in the acceleration.

Checks

Does it make sense?

If the plates were not moved, E′=EE' = E and the formula gives a=0a = 0, as it should for droplets at rest.

If the plates are very close, E′E' is very big and aa is big and upward, as a strong field would give.

Conclusion

a=g(E′E−1)a = g\left(\dfrac{E'}{E} - 1\right)

Both droplets rise with the same acceleration g(E′E−1)g\left(\dfrac{E'}{E} - 1\right). That is option (3).

The answer is (3).

The quotes give the field intensity, the force F=EqF = Eq and the field as the potential gradient. That the field between two parallel plates is VV over dd, and that qm\dfrac{q}{m} is the same for the two droplets because they hang in balance, is our reasoning from them. We ignore the buoyancy of the air and the pull of the droplets on each other, as the question says.

Teacher's note

A droplet at rest in a field has qE=mgqE = mg, so its qm\dfrac{q}{m} is gE\dfrac{g}{E}. When the field changes, the acceleration is g(E′E−1)g\left(\dfrac{E'}{E} - 1\right).

The mass is not in this, so droplets of different mass move together.

Exam tip

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