Change of State
AdvancedDuring a change of state the temperature stays constant: melting and vaporisation absorb energy, freezing and condensation release it. Use Q = ml with water's specific latent heats of 3.34 × 10⁵ (fusion) and 2.26 × 10⁶ J kg⁻¹ (vaporisation); the plateau of a heating curve marks a change of state.
- During changes of state (melting, freezing, vaporisation, condensation) the temperature stays constant
- Melting and vaporisation absorb energy; freezing and condensation release it — latent heat changes particle potential energy
- Q = ml; for water l_f = 3.34 × 10⁵ J kg⁻¹ and l_v = 2.26 × 10⁶ J kg⁻¹
文體小知識:科學知識說明文——說明熔解、凝固、汽化、凝結與蒸發的現象和微觀解釋,並用比潛熱處理計算。
§Text Passage
1Matter exists in three states: solid, liquid and gas. Particles in a solid are packed closely and can only vibrate about fixed positions; liquid particles are slightly further apart and can slide past one another; gas particles are far apart and fly about freely. States can change into one another: solid to liquid is melting, liquid to solid is freezing, liquid to gas is vaporisation, and gas to liquid is condensation.
2A change of state has a striking feature: the temperature stays constant throughout. Heat ice and, once it reaches its melting point of 0°C, the ice-water mixture stays at 0°C during the whole melting process; only when all the ice has melted does the temperature climb again. This 'non-heating' energy goes into the potential energy between particles, and physics calls it latent heat.
3The specific latent heat of fusion is the energy needed to melt 1 kg of a solid completely; for water it is about 334000 J kg⁻¹. The specific latent heat of vaporisation is the energy needed to vaporise 1 kg of a liquid completely; for water it is about 2260000 J kg⁻¹, far larger than fusion, because vaporisation must pull the particles completely apart against much stronger intermolecular forces.
4Latent heat is calculated with the formula: heat equals mass times specific latent heat. For example, turning 0.5 kg of water at 100°C completely into steam takes 0.5 × 2260000 ≈ 1130000 J — several times the energy needed to warm the same water from its ice point to its boiling point, showing how energy-hungry vaporisation is.
5Evaporation is vaporisation at any temperature below the boiling point: individual particles with exceptionally high kinetic energy escape from the liquid surface, carrying extra energy away, so the liquid left behind cools — that is why evaporation feels cold. Sweating cools us and rubbing alcohol feels cool on the skin by the same principle; the higher the temperature, the larger the surface area and the faster the air moves, the quicker evaporation is.
1Summary 重點摘要
During a change of state the temperature stays constant: melting and vaporisation absorb energy, freezing and condensation release it. Use Q = ml with water's specific latent heats of 3.34 × 10⁵ (fusion) and 2.26 × 10⁶ J kg⁻¹ (vaporisation); the plateau of a heating curve marks a change of state.
2Vocabulary cards Vocabulary
The form matter takes — solid, liquid or gas — each with its own particle arrangement and motion.
The temperature at which a solid melts; the freezing point equals it, e.g. 0°C for ice.
The temperature at which a liquid boils; water boils at 100°C under standard atmospheric pressure.
The interconversion between solid and liquid; melting absorbs energy, freezing releases it.
The interconversion between liquid and gas; vaporisation absorbs energy, condensation releases it.
The energy absorbed or released during a change of state while the temperature stays unchanged.
The energy needed to melt 1 kg of a solid completely; for water, 3.34 × 10⁵ J kg⁻¹.
The energy needed to vaporise 1 kg of a liquid completely; for water, 2.26 × 10⁶ J kg⁻¹.
Vaporisation below the boiling point, in which the most energetic particles escape from the surface; it has a cooling effect.
A graph of temperature against heating time; each plateau marks a change of state.
3Step by step Steps
- Step 1: Three states in particle termsDescribe changes of state with the particle picture. Particles in a solid are tightly packed and orderly, vibrating about fixed positions, so solids keep both shape and volume; liquid particles stay close but can slide past each other, so liquids keep volume but not shape; gas particles are far apart and fly freely, filling the whole container. A change of state is a change of particle arrangement and separation. For example, when ice melts, particles go from orderly vibration to sliding about; when water boils into steam, the particles break apart completely and the volume expands enormously.
- Step 2: Melting and freezing — a pair of oppositesMelting turns a solid into a liquid and absorbs energy; freezing turns a liquid into a solid and releases energy. Both happen at the same temperature — the melting point (which equals the freezing point). For ice it is 0°C. For example, leave an ice-water mixture in a warm room and the ice keeps melting and absorbing heat; while any ice remains, the mixture stays at exactly 0°C. Conversely, water freezing releases latent heat — orchard farmers spray water on frosty nights, and the heat released as the water freezes protects the fruit from frost damage.
- Step 3: Vaporisation and condensation — the energetic pairVaporisation turns liquid into gas and absorbs a great deal of energy; condensation turns gas into liquid and releases exactly as much. At standard atmospheric pressure water boils at 100°C, with vigorous vaporisation throughout the liquid and at the surface. For example, steam scalds are often worse than scalds from boiling water at the same temperature: the steam first condenses on the skin, releasing its specific latent heat of 2.26 × 10⁶ J kg⁻¹, then cools — so the total energy delivered far exceeds that of the same mass of boiling water. This is also why pressurised steam carries such enormous energy.
- Step 4: Specific latent heat and Q = mlThe specific latent heat l is the energy needed to change the state of 1 kg of a substance completely, in J kg⁻¹: use the specific latent heat of fusion l_f for melting and of vaporisation l_v for boiling, both with Q = ml. For water, l_f = 3.34 × 10⁵ J kg⁻¹ and l_v = 2.26 × 10⁶ J kg⁻¹. For example, turning 0.5 kg of water at 100°C fully into steam takes Q = ml = 0.5 × 2.26 × 10⁶ = 1.13 × 10⁶ J, while heating the same 0.5 kg of water from 0°C to 100°C needs only 0.5 × 4200 × 100 = 210000 J — vaporisation costs more than five times as much.
- Step 5: The heating curve and its plateausHeat ice steadily and record temperature against time to obtain a heating curve: first the ice warms up, then at 0°C comes the first plateau — the ice is melting, and all the latent heat goes into raising particle potential energy, so the temperature holds; once melted, the water warms again until 100°C brings the second plateau — the water is boiling. For example, an exam question shows a curve with two plateaus: the plateau temperatures are the melting and boiling points, and the plateau lengths reflect how much latent heat is involved. Remember: plateau = change of state, temperature constant — the heating has not stopped.
- Step 6: Evaporation and coolingEvaporation is vaporisation below the boiling point: only particles at the surface with exceptionally high kinetic energy can break free and fly away. These escapees take extra energy with them, so the average kinetic energy of the liquid left behind falls and its temperature drops — the cooling effect of evaporation. Evaporation speeds up with higher temperature, larger surface area, faster air movement and lower humidity. For example, sponging a feverish patient with warm water cools the body as the water evaporates; a dog pants on a hot day to lose heat as its saliva evaporates.
- Step 7: Combined calculations — warming and changing state togetherHarder questions chain Q = mcΔT with Q = ml: warm first, change state, then warm again, adding the energies of each stage. For example, turning 0.2 kg of ice at 0°C into water at 25°C takes two stages — melting first: Q₁ = ml_f = 0.2 × 3.34 × 10⁵ = 66800 J; then warming the water from 0°C to 25°C: Q₂ = mcΔT = 0.2 × 4200 × 25 = 21000 J; total Q = 66800 + 21000 = 87800 J. Listing each stage with its own formula and adding them up is the safe strategy for such questions.
4Diagrams Diagrams
5Worked example Example
Example: at standard atmospheric pressure, 0.5 kg of water at 100°C is completely vaporised into steam at 100°C. Given the specific latent heat of vaporisation of water l_v = 2.26 × 10⁶ J kg⁻¹, find the energy required, and explain why the temperature stays at 100°C throughout.
- Choose the formula: the process is a change of state with no temperature change, so use Q = ml (vaporisation uses l_v)
- Substitute: Q = ml_v = 0.5 × 2.26 × 10⁶
- Calculate: Q = 1.13 × 10⁶ J
- Explain the plateau: during vaporisation all the absorbed energy raises the potential energy of the particles (pulling them apart); the average kinetic energy is unchanged, so the temperature stays at 100°C
- Answer: The energy required is Q = ml_v = 0.5 × 2.26 × 10⁶ = 1.13 × 10⁶ J. The temperature stays at 100°C because all the latent heat absorbed goes into particle potential energy while the average kinetic energy is unchanged; the temperature rises again only after all the liquid has become steam.
6Common mistakes Mistakes
7Quick check Quick check
Q1Why does the temperature stay constant during a change of state?
Q2Calculate the energy needed to melt 0.2 kg of ice at 0°C completely.
Q3Why are steam scalds worse than scalds from water at the same temperature?
Q4What does a plateau on a heating curve represent?
Q5Why does evaporation cool?
8Recap Recap
- During changes of state (melting, freezing, vaporisation, condensation) the temperature stays constant
- Melting and vaporisation absorb energy; freezing and condensation release it — latent heat changes particle potential energy
- Q = ml; for water l_f = 3.34 × 10⁵ J kg⁻¹ and l_v = 2.26 × 10⁶ J kg⁻¹
- A plateau on a heating curve means a change of state; its temperature is the melting or boiling point
- Evaporation happens below the boiling point; escaping high-energy particles cool the liquid — used for cooling