Physical and chemical changes are accompanied by a change in energy, typically in the form of heat. The energy change associated with a physical process provides a quantitative measure of the strength of intermolecular forces. The change in energy at constant pressure is called the enthalpy change, denoted by . It is expressed in units of . A key characteristic of a phase change is that the temperature of the substance remains constant while heat is added or removed.
Molar heat of fusion is the amount of heat required to convert one mole of a solid into its liquid state at its melting point. It represents the energy needed to overcome the forces holding the particles in the fixed crystal lattice.
The molar heat of fusion for ice is . The positive sign indicates that this is an endothermic process (heat is absorbed).
Molar heat of vaporization is the amount of heat required to convert one mole of a liquid into its vapor (gas) state at its boiling point. This energy is used to overcome the intermolecular attractions that hold the liquid molecules together.
The molar heat of vaporization for water is .
Some solids directly convert into vapors without passing through the liquid phase. The heat required to convert one mole of a solid directly into its vapors at a specific temperature and pressure is called the molar heat of sublimation. According to Hess's Law, the heat of sublimation is the sum of the heat of fusion and heat of vaporization.
When a solid melts, there is a relatively small change in the intermolecular distances and potential energy of the particles (atoms, molecules, or ions). However, when a liquid evaporates, the particles undergo a large change in their intermolecular distances as they move far apart in the gas phase. This results in a significant increase in their potential energy.
Consequently, the heat of vaporization is much greater than the heat of fusion for the same substance because more energy is required to completely separate the molecules than to simply allow them to move past one another in the liquid state.
The strength of these forces also determines the physical state at room temperature. For example, in Halogens→, larger atoms have stronger London dispersion forces.
In 1888, the Austrian botanist Friedrich Reinitzer discovered a unique state of matter while studying an organic compound, cholesteryl benzoate. He observed that when this solid was heated, it first turned into a milky, turbid liquid at and then into a clear liquid at . Upon cooling, the reverse process occurred. This turbid intermediate state is known as a liquid crystal.
The liquid crystal state exists between the melting temperature and a "clearing" temperature.
Properties of Liquid Crystals:
The unique ability of liquid crystals to change their molecular structure in response to external factors like electric fields and temperature makes them highly useful.
| Property | Crystalline Solids | Liquid Crystals | Pure Liquids |
|---|---|---|---|
| Molecular Arrangement | Well-ordered, repeating 3D lattice. Long-range order. | Molecules have some degree of order (e.g., parallel alignment) but not fixed positions. | Completely random arrangement. No long-range order. |
| Flow | Cannot flow; rigid structure. | Can flow like a liquid. | Flow freely. |
| Optical Properties | Anisotropic — properties vary with direction. | Anisotropic — exhibit direction-dependent optical properties. | Isotropic — properties same in all directions. |
| Melting Behaviour | Sharp, definite melting point. | Two transition temperatures: melting point and clearing temperature. | No melting point (already liquid). |
| Shape | Definite shape. | No definite shape; takes shape of container. | No definite shape; takes shape of container. |
| Example | NaCl, ice, quartz | Cholesteryl benzoate, LCD materials | Water, ethanol, benzene |