2022 A/L Physics Past Paper · Question 47 (English Medium)

Moisture removed by an air conditioner and the final relative humidity of the air

Ambient air at 30 ∘C30\ ^\circ\text{C} and relative humidity (RH) 90%90\% is cooled to 10 ∘C10\ ^\circ\text{C} and some of the moisture in air is removed by an air-conditioning plant. Then this air is heated to 20 ∘C20\ ^\circ\text{C} and passed to a computer laboratory. If the values of saturated water vapour pressure at temperatures 10 ∘C10\ ^\circ\text{C}, 20 ∘C20\ ^\circ\text{C} and 30 ∘C30\ ^\circ\text{C} are given by aa, bb and cc respectively, what is the ratio of moisture removed from the plant and the final relative humidity (RH) of the air at 20 ∘C20\ ^\circ\text{C}?

  1. (1) 0.9c−a0.9c\dfrac{0.9c - a}{0.9c}, a×100b%\dfrac{a \times 100}{b}\%
  2. (2) 0.9c−a0.9c\dfrac{0.9c - a}{0.9c}, c×100b%\dfrac{c \times 100}{b}\%
  3. (3) 0.9c−ac\dfrac{0.9c - a}{c}, a×100b%\dfrac{a \times 100}{b}\%
  4. (4) c−ac\dfrac{c - a}{c}, b×100c%\dfrac{b \times 100}{c}\%
  5. (5) c−ac\dfrac{c - a}{c}, a×100c%\dfrac{a \times 100}{c}\%
Answer and explanation

Answer: (1) 0.9c−a0.9c\dfrac{0.9c - a}{0.9c}, a×100b%\dfrac{a \times 100}{b}\%

Given information

What we know:

Air at 30 ∘C30\ ^\circ\text{C} has a relative humidity of 90%90\%.

The plant cools it to 10 ∘C10\ ^\circ\text{C} and removes some water. Then the air is heated to 20 ∘C20\ ^\circ\text{C}.

The saturated vapour pressures are aa at 10 ∘C10\ ^\circ\text{C}, bb at 20 ∘C20\ ^\circ\text{C} and cc at 30 ∘C30\ ^\circ\text{C}.

There are no numbers, so we keep the letters. Later we check with sample values.

What the question asks

We want: the share of the moisture removed, and the final RH at 20 ∘C20\ ^\circ\text{C}.

The options show the moisture removed as a fraction of the moisture that was in the air at the start.

What each letter means:

aa, bb, cc (Pa\text{Pa}): the saturated water vapour pressure at 10 ∘C10\ ^\circ\text{C}, 20 ∘C20\ ^\circ\text{C} and 30 ∘C30\ ^\circ\text{C}.

pp (Pa\text{Pa}): the vapour pressure of the water vapour in the air.

RHRH (%\%): the relative humidity, how full the air is of water vapour.

Relevant theory

What is happening:

At the start the air is not full of vapour. At 90%90\% RH its vapour pressure is 0.9c0.9c.

The plant cools the air to 10 ∘C10\ ^\circ\text{C}. Cold air can hold less vapour. So the vapour that does not fit turns into water and is taken out.

The air leaves the plant just full of vapour at 10 ∘C10\ ^\circ\text{C}. Its vapour pressure is aa.

Then the air is heated to 20 ∘C20\ ^\circ\text{C}. Nothing is added or removed, so the vapour in the air stays as it was. But warm air can hold more, so the air is no longer full.

The options use only aa, bb and cc. So we take the air to stay at one total pressure, and the amount of vapour to go with its vapour pressure.

The relative humidity of a given volume of air at some temperature is defined as the ratio of the mass ( m) of water vapour present in that volume to the mass ( m0) of water vapour present in the same volume at the same temperature when it is saturated with water vapour.

p = vapour pressure at the given temperature

The other way is by reducing its temperature to reach the saturation point.

The first quote says that relative humidity is the vapour in the air compared with the vapour the same air would hold when full, at the same temperature.

The second quote names pp as the vapour pressure at the given temperature. Pressure and amount of vapour go together, so we can use pressures in place of amounts.

The third quote says that cooling is one way to make air full of vapour.

For example, a cold glass of water on a warm day. The air touching the glass is cooled. It cannot hold all its vapour, so tiny drops of water form on the outside of the glass.

Required equations

p1=0.9 cp_1 = 0.9\,c

p2=ap_2 = a

p1−p2p1=0.9c−a0.9c\dfrac{p_1 - p_2}{p_1} = \dfrac{0.9c - a}{0.9c}

RH=ab×100%RH = \dfrac{a}{b} \times 100\%

Applying it to this question

Every pressure in the fractions is in Pa\text{Pa}, so each fraction has no unit. The share removed is a number between 00 and 11, and RHRH is a percentage.

The cooling makes the air full only if 0.9c0.9c is bigger than aa. It is, because air at 30 ∘C30\ ^\circ\text{C} can hold much more vapour than air at 10 ∘C10\ ^\circ\text{C}.

0.9c0.9c

p1p_1

aa

p2p_2

p1−p2p1=0.9c−a0.9c\dfrac{p_1 - p_2}{p_1} = \dfrac{0.9c - a}{0.9c}

p3p_3

RH=ab×100%RH = \dfrac{a}{b} \times 100\%

Reasoning and calculation

The share removed is 0.9c−a0.9c\dfrac{0.9c - a}{0.9c} and the final RH is a×100b%\dfrac{a \times 100}{b}\%.

That is the pair in option (1).

Checks

a∗100/ba * 100 / b

Does it make sense?

With the sample values, about two thirds of the vapour is taken out and the air ends at about 52%52\% RH. Air that is 90%90\% full at 30 ∘C30\ ^\circ\text{C}, cooled, dried and then warmed to 20 ∘C20\ ^\circ\text{C}, feels drier.

The final RH is below 100%100\%, as it must be for air that is not full.

The sample values are close to real ones but they are only for the check. The answer is in the letters.

Conclusion

0.9c−a0.9c, a×100b%\dfrac{0.9c - a}{0.9c},\ \dfrac{a \times 100}{b}\%

The share removed is 0.9c−a0.9c\dfrac{0.9c - a}{0.9c} and the final RH is a×100b%\dfrac{a \times 100}{b}\%.

The answer is (1).

Write the vapour pressure at each stage. At the start it is RHRH times the saturated pressure. If the cooling takes water out, the air is full, so it equals the saturated pressure at the cold temperature.

Heating without adding or removing vapour leaves the vapour pressure the same. Divide it by the saturated pressure at the new temperature for the new RH.

Exam tip

தமிழ் · සිංහල