2023 A/L Physics Past Paper · Question 09 (English Medium)

Density of a gas against its temperature at a steady pressure

If the pressure of a given mass of an ideal gas is kept constant, the variation of its density ρ\rho with the absolute temperature TT is best represented by

  1. (1) Graph (1)
  2. (2) Graph (2)
  3. (3) Graph (3)
  4. (4) Graph (4)
  5. (5) Graph (5)
Answer and explanation

Answer: (5) Graph (5)

What the question asks

We want: the graph of the density ρ\rho of the gas against its absolute temperature TT, when the pressure stays the same.

What each letter means:

ρ\rho (kg m−3\text{kg m}^{-3}): the density of the gas.

TT (K\text{K}): the absolute temperature of the gas.

mm (kg\text{kg}): the mass of the gas. It is given and does not change.

VV (m3\text{m}^3): the volume of the gas.

pp (Pa\text{Pa}): the pressure of the gas. It does not change.

There are no numbers. We keep the letters, and later we check with sample values: 300 K300\ \text{K} at aa and 600 K600\ \text{K} at bb.

Relevant theory

What is happening:

The gas is warmed, and the pressure on it stays the same. So the gas spreads out and takes more room.

The mass of the gas stays the same. The same mass in a bigger volume is spread thinner, so its density is smaller.

We need to say how much smaller.

The volume of a fixed mass of a gas is directly proportional to its absolute temperature, provided the pressure remains constant.

The mass of a unit volume of a substance is termed its density.

The first quote is Charles' law. It says the volume is in proportion to the absolute temperature, when the pressure stays the same.

The second quote tells us what density is: mass in each unit of volume.

For example, think of a hot air balloon. The burner warms the air inside, and the air spreads out into a bigger space. The same air fills more room, so each cubic metre holds less of it. The balloon then floats up.

Required equations

V=kTV = kT

ρ=mV\rho = \dfrac{m}{V}

ρ=mkT\rho = \dfrac{m}{kT}

ρ∝1T\rho \propto \dfrac{1}{T}

Reasoning and calculation

300300

TaT_a

600600

Tb=2×300T_b = 2 \times 300

0.50.5

ρbρa=TaTb=300600\dfrac{\rho_b}{\rho_a} = \dfrac{T_a}{T_b} = \dfrac{300}{600}

When TT doubles, ρ\rho halves. It does not go to zero. It keeps getting smaller as TT grows.

Check the five graphs.

Graphs (1), (2) and (4) rise. A warmed gas gets thinner, so they cannot be right.

Graph (3) falls along a straight line. The density would fall by the same amount for each step of TT, but it has to halve when TT doubles.

Graph (5) falls steeply at first and then slowly. It matches.

Checks

t1/t2t1 / t2

Does it make sense?

A gas gets thinner when it is warmed at a steady pressure, like the air in the hot air balloon. So the density has to fall as TT rises.

The density has no way to become zero, because the gas is still there. So the graph gets closer and closer to the TT axis without touching it, and that is graph (5).

Conclusion

graph (5)\text{graph }(5)

The density falls steeply at first and then slowly. The graph is (5).

The answer is (5).

For a gas at a steady pressure, the volume goes with TT, and the density is mass over volume.

So the density goes with 1T\dfrac{1}{T}. Look for the graph that falls steeply and then slowly.

Exam tip

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