2021 A/L Physics Past Paper · Question 30 (English Medium)

Change in internal energy of heated air

Air is trapped in a well-insulated container by a frictionless piston as shown in the figure. The air is heated by a coil of resistance 100 Ω100\ \Omega passing a current of 1 A1\ \text{A} for 55 minutes. The air expands from a volume of 0.4 m30.4\ \text{m}^3 to 0.5 m30.5\ \text{m}^3 at a constant pressure of 150 kPa150\ \text{kPa} during the heating process. The change in internal energy of the air is,

  1. (1) 5 kJ5\ \text{kJ}
  2. (2) 15 kJ15\ \text{kJ}
  3. (3) 30 kJ30\ \text{kJ}
  4. (4) 45 kJ45\ \text{kJ}
  5. (5) 60 kJ60\ \text{kJ}
Answer and explanation

Answer: (2) 15 kJ15\ \text{kJ}

Given information

We know:

Coil: R=100 ΩR = 100\ \Omega, I=1 AI = 1\ \text{A}, t=5 min=300 st = 5\ \text{min} = 300\ \text{s}.

Air: constant pressure p=150 kPa=1.5×105 Pap = 150\ \text{kPa} = 1.5 \times 10^5\ \text{Pa}, volume from 0.4 m30.4\ \text{m}^3 to 0.5 m30.5\ \text{m}^3.

The container is well insulated, so no heat leaks out.

What each letter means:

RR (Ω\Omega): resistance of the coil, how hard it is for current to pass.

II (A\text{A}): current, how much charge flows each second.

tt (s\text{s}): time, how long the coil is on.

pp (Pa\text{Pa}): pressure, how hard the air pushes on the piston.

VV (m3\text{m}^3): volume, the space the air fills.

ΔQ\Delta Q (J\text{J}): heat that the coil gives to the air.

ΔW\Delta W (J\text{J}): work that the air does when it pushes the piston up.

ΔU\Delta U (J\text{J}): change in internal energy, the energy that stays inside the air.

What the question asks

We want: the change ΔU\Delta U in the internal energy of the air.

The plan: find the heat from the coil, find the work done by the air, then use the first law.

Relevant theory

Heat is mainly liberated when a current passes through a resistor and this is known as "joule heating".

In a system, if the net exchange of heat is ∆Q, the change of internal energy is ∆U and the amount of work done is ∆W then,

∆ W = p.∆V (under constant pressure)

Required equations

ΔQ=I2Rt\Delta Q = I^2 R t

ΔW=p ΔV\Delta W = p\,\Delta V

ΔQ=ΔU+ΔW\Delta Q = \Delta U + \Delta W

Applying it to this question

For example:

Amma cooks rice in a pot with a heavy lid. The flame gives the pot heat. That is the heat from the coil, ΔQ\Delta Q.

The steam pushes the heavy lid up. That is the work the air does when it pushes the piston up, ΔW\Delta W.

The rest of the heat makes the water hotter. That is the energy that stays inside the air, ΔU\Delta U.

ΔQ=ΔU+ΔW\Delta Q = \Delta U + \Delta W

In words: heat from the flame=heat that warms the water+work that lifts the lid. Heat in=energy kept+work doneheat\,from\,the\,flame = heat\,that\,warms\,the\,water + work\,that\,lifts\,the\,lid.\,Heat\,in = energy\,kept + work\,done

The coil gives more heat for a bigger current, a bigger resistance or a longer time. The air does more work for a bigger pressure or a bigger change of volume.

3000030000

ΔQ=12×100×300\Delta Q = 1^2 \times 100 \times 300

0.10.1

ΔV=0.5−0.4\Delta V = 0.5 - 0.4

1500015000

ΔW=1.5×105×0.1\Delta W = 1.5 \times 10^5 \times 0.1

ΔU=ΔQ−ΔW=30000−15000\Delta U = \Delta Q - \Delta W = 30000 - 15000

ΔQ\Delta Q and ΔW\Delta W are both in joules, so ΔU\Delta U is in joules: 15000 J=15 kJ15000\ \text{J} = 15\ \text{kJ}.

Reasoning and calculation

Half of the heat goes into pushing the piston up. The other half stays in the air as internal energy.

ΔU=15 kJ\Delta U = 15\ \text{kJ}. The answer is (2).

Checks

i∗i∗r∗t−p∗vi * i * r * t - p * v

Does it make sense?

The air expands, so it does work and ΔW\Delta W is positive. So ΔU\Delta U must be less than the heat supplied, 30 kJ30\ \text{kJ}.

The air is heated at constant pressure, so its temperature rises. So ΔU\Delta U must be positive. 15 kJ15\ \text{kJ} fits both.

Conclusion

ΔU=I2Rt−pΔV=15 kJ\Delta U = I^2Rt - p\Delta V = 15\ \text{kJ}

ΔQ=30 kJ\Delta Q = 30\ \text{kJ}, ΔW=15 kJ\Delta W = 15\ \text{kJ}.

ΔU=30−15=15 kJ\Delta U = 30 - 15 = 15\ \text{kJ}. The answer is (2).

In a heating question with a moving piston, the heat splits two ways: work on the piston and a rise in internal energy.

Change minutes to seconds before using I2RtI^2Rt.

Exam tip

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