State the melting and boiling points of water at 1 atm and describe the four phase‑change processes in terms of energy flow and particle behaviour.
1 atm = 101.3 kPa. All temperature values given below refer to this pressure unless otherwise noted.
Energy absorbed: latent heat of fusion.
Temperature remains constant because the absorbed energy is used to break the ordered intermolecular bonds of the solid.
Particle view: the rigid lattice of ice becomes a less‑ordered arrangement of water molecules that can move past one another.
Energy absorbed: latent heat of vaporisation.
Temperature stays at the boiling point while the supplied energy overcomes the attractive forces between molecules and creates vapour bubbles that rise to the surface.
Particle view: molecules gain enough kinetic energy to escape the liquid phase.
Can occur at any temperature; the rate increases with temperature, surface area and wind.
The most energetic surface molecules leave the liquid, leaving the remaining molecules with a lower average kinetic energy – a cooling effect.
Energy released: latent heat of vaporisation.
Fast‑moving gas particles lose kinetic energy, collide, and form intermolecular bonds, producing a liquid. The surrounding environment gains the released heat.
Energy released: latent heat of fusion.
As the temperature falls to the freezing point, liquid molecules lose kinetic energy, arrange into a regular lattice and release heat to the surroundings.
Key point: During melting and boiling the temperature of the substance does not rise because the supplied energy is used to break intermolecular bonds – this is called latent heat.
| Phase change | Temperature (°C) | Temperature (K) |
|---|---|---|
| Melting (solid → liquid) | 0 °C | 273.15 K |
| Boiling (liquid → gas) | 100 °C | 373.15 K |
These two fixed points define the Celsius scale: 0 °C is the melting point of ice and 100 °C is the boiling point of water at 1 atm.
| Feature | Boiling | Evaporation |
|---|---|---|
| Where it occurs | Throughout the bulk; bubbles form inside the liquid and rise to the surface. | Only at the liquid–air interface. |
| Temperature requirement | Liquid must reach its boiling point so that vapour pressure = external pressure. | Can occur at any temperature; rate rises with temperature, surface area and wind. |
| Energy flow | Large amount of latent heat of vaporisation absorbed. | High‑energy surface molecules escape; the remaining liquid loses kinetic energy (cooling). |
| Visible sign | Rapid formation of bubbles throughout the liquid. | Gradual loss of liquid, no bubbles. |
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