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GRADE 8 · CHANGE IN STATE OF AGGREGATION

Boiling and vaporization

Boiling temperature, pressure and specific latent heat of vaporization.

22 minutes5 theory cards
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Understanding step by step

Water was already evaporating before it was heated. What new process occurs when vapour bubbles start growing in a saucepan? Why does this begin at a lower temperature in the mountains?

Vapour forms below the surfaceQwater pushesfrom outsideThe bubble must withstand this pressure
During boiling, vapour forms in bubbles inside the liquid. Blue arrows show their rise. The red arrow on the right points from the surrounding water towards the bubble boundary: the pressure inside must withstand this local pressure. Energy entering the water is shown below.

Vapour inside the liquid

In ordinary evaporation, molecules leave the water's upper surface. During boiling, vapour also forms inside the liquid in growing bubbles, each with its own liquid–vapour boundary. Boiling is vaporization involving the formation and growth of vapour bubbles within the liquid. Small bubbles of dissolved air can appear before boiling, so seeing any bubble at all is not sufficient evidence.

Heat supplied: Q = Lm
During boiling, vapour bubbles grow within the liquid and rise. At a fixed external pressure, the temperature of a pure boiling liquid does not rise.

When can bubbles grow?

The surrounding water compresses a bubble. For sustained growth, the pressure inside must withstand this compression. Saturated vapour pressure increases with temperature, so heating makes growth possible. In a simple shallow-vessel model, boiling starts when vapour pressure equals the pressure above the liquid. At depth, the water column adds pressure, while surface tension matters for very small bubbles.

ColderHottervapour pressuretoo lowenough pressurebubble growsHigher temperature → higher vapour pressure
Two regions of water at the same local external pressure. In colder water, the vapour pressure is insufficient and the bubble contracts; in hotter water, it can grow. Arrows show the boundary moving and start or end on it. This simple model neglects the extra pressures due to surface tension and depth.

Why mountains are different

Predict: if the pressure above water is reduced, must it be heated as much? No: vapour can sustain bubbles at a lower pressure and therefore a lower temperature. Water thus boils below 100 °C in the mountains and above this temperature in a pressure cooker at higher pressure. Boiling does not imply one fixed temperature under all conditions. About 100 °C applies to pure water at ordinary atmospheric pressure.

Water's boiling temperaturep < p₀p ≈ p₀p > p₀MountainsSea levelPressure cooker< 100 °C≈ 100 °C> 100 °CCompared with normal pressure p₀
For pure water, the pressure above the liquid is below normal in the mountains, close to normal at sea level, and above normal in an operating pressure cooker. The boiling temperature is therefore below, approximately at, and above 100 °C respectively. p₀ denotes normal atmospheric pressure, not the vapour pressure at any temperature.

Energy for the change of state

After boiling begins, the heater continues to supply energy. This energy separates the liquid's particles and increases the substance's volume, displacing its surroundings. The specific latent heat of vaporization L is the energy needed to turn 1 kg of liquid into vapour at the specified transition temperature, measured in J/kg. A larger L means more energy for the same mass. L can also change when boiling conditions change.

Water at atmospheric pressure1 кг of water≈ 100 °C≈ 2,3 МДж1 кг of vapour≈ 100 °CL: energy per 1 кг, unit Дж/кг
At atmospheric pressure, 1 kg of water at about 100 °C turns into 1 kg of vapour at the same temperature. With the rounded value L ≈ 2,3 МДж/кг, about 2.3 MJ is needed. Molecules are conserved; energy overcomes their attraction and enables expansion. Identical dots represent molecules; volumes are not to scale.

Accounting for the vapour mass

For liquid already at its boiling temperature, each kilogram vaporized requires L joules: Q = Lm. Doubling the vapour mass doubles Q; half the mass needs half the energy. If no vapour forms during a stage, its Lm contribution is zero. At constant pressure, a pure boiling liquid stays at approximately the same temperature: increasing the energy supply mainly speeds up vapour formation until the liquid has boiled away.

Q = L · mboilsmass mbecame vapourtemperature stays constantuntil all the water boils away
Multiply the specific latent heat by the mass that becomes vapour. While the liquid boils at constant pressure, its temperature remains approximately constant.

Returning to liquid

What happens in the reverse change? When vapour condenses under the same conditions, it releases energy of magnitude Lm: the transition energy that previously had to be supplied. If the resulting liquid then cools, it releases additional energy described by cmΔT, with a negative sign for the liquid. Do not combine these stages into a single formula: condensation changes the state; the subsequent cooling changes the temperature.

VapourLiquidColderTкипTкипT < TкипMass m is conservedQ₁ = −LmQ₂ = cmΔTOn cooling, ΔT < 0
The same mass m first condenses at the transition temperature, releasing Q₁ = −Lm; the resulting liquid may then cool with Q₂ = cmΔT. Grey arrows connect the states. In the first stage, the energy magnitude equals that for the reverse vaporization; in the second, ΔT is negative. Vapour and water volumes are not to scale.

The starting temperature matters

Start with cold water and aim to turn only part of its mass into vapour. First, all the water being heated receives energy cmΔT. Then Lm is needed for the mass that actually vaporizes. Add these contributions; if all the water vaporizes, the masses in the two stages are equal. If some energy goes to the vessel and air, the source must supply more. Such losses may be neglected only within the model adopted for the problem.

Two successive stagesfrom Tнач to TкипQ₁ = cmвΔTwater → vapourQ₂ = LmпQ = Q₁ + Q₂mв: all water; mп: vapour mass
First heat all the water of mass mв from Tнач to Tкип; then turn mass mп into vapour at the same pressure. Add the energies. If only part of the water vaporizes, mп is less than mв, so the masses in the two formulas can differ. Account for losses as stated in the problem.

A portion of vapour

Turn 0.2 kg of water at its boiling temperature into vapour. L = 2,3 МДж/кг. Find the heat required.

L = 2,3 МДж/кгwater, 0,2 кгvapour, 0,2 кгTкипTкипFind the transition heat Q
The initial 0.2 kg of water is already at its boiling temperature and must all become vapour. Given L = 2,3 МДж/кг, find the heat for the transition itself. The initial state is on the left and the required final state on the right. No numerical temperature is specified; volumes are schematic and dots on the right represent vapour molecules.

Worked example · 1

The water is already at its boiling temperature. Energy is therefore needed only to change 0.2 kg of liquid into vapour, with no preliminary heating.

L = 2,3 МДж/кгwater, 0,2 кгvapour, 0,2 кгTкипTкипNo heating to boiling is neededTransition needed: Q = Lm
The initial and final states of the 0.2 kg portion and the given L are unchanged. The water is already at Tкип, so no separate heating to that temperature is needed. Calculate only the change into vapour using Q = Lm.

Worked example · 2

Q = Lm = 2,3·0,2 = 0,46 МДж = 460 кДж. Unit check: МДж/кг · кг = МДж.

L = 2,3 МДж/кгwater, 0,2 кгvapour, 0,2 кгTкипTкипQ = Lm2,3 · 0,2 = 0,46 МДжQ = 460 кДж
On the same diagram, for mass 0.2 kg and L = 2,3 МДж/кг, we obtain Q = 0,46 МДж. Kilograms cancel, and 0.46 MJ equals 460 kJ. Mass and transition temperature are unchanged on both sides.

Worked example · 3

The mass is one fifth of a kilogram, so the energy is one fifth of 2.3 MJ. Constant temperature is consistent with this: the water's state and volume change.

L = 2,3 МДж/кгwater, 0,2 кгvapour, 0,2 кгTкипTкип460 кДжDuring boiling, T ≈ const and p = constEnergy goes into vaporization
The same 0.2 kg of water becomes 0.2 kg of vapour after receiving 460 kJ for the transition. At constant pressure, a pure substance remains near Tкип during boiling. The right-hand state is vapour just as the transition ends; subsequent heating of the vapour is not included.

Check the result

460 kJ. This energy turns the specified portion of boiling water into vapour under the given conditions.

Key idea · 1

Vapour bubbles grow when their internal pressure can withstand the surrounding pressure.

Key idea · 2

Boiling temperature depends on pressure, so 100 °C applies to specific conditions.

Key idea · 3

Q = Lm gives the energy to turn the required mass into vapour; account for preliminary heating and losses separately.

What comes next

Expanding vapour can push a piston or turbine blades. The next lesson connects thermal processes with mechanical work.

Basic Concepts

3 concepts

Boiling

Intense vaporization throughout a liquid, with vapour bubbles forming and growing within it.

Boiling begins when the saturated vapor pressure is equal to the external pressure.

Specific latent heat of vaporization

The energy required to convert a unit mass of liquid into vapor at the boiling point.

Condensing the same mass of vapour releases the same magnitude of energy.

Boiling point and pressure

The boiling point decreases as the external pressure decreases and increases as it increases.

High in the mountains, water boils below one hundred degrees, and in a pressure cooker, increased pressure allows it to heat up more.

Physical quantities

1 magnitude

Specific latent heat of vaporization

L

The energy required to convert a unit mass of liquid into vapor during boiling.

Unit: joule per kilogram · \frac{\mathrm{Дж}}{\mathrm{кг}}

Lesson formulas

1 formula

Heat of vaporization

Q = Lm

During boiling, the heat required equals the specific latent heat of vaporization multiplied by the mass of liquid vaporized.

Problems on this topic

Statements, answer options and the walkthrough.