An ionic compound has a giant ionic lattice structure. The ions are arranged in a lattice such that there is maximum electrostatic forces of attraction between the oppositely charged ions (e.g., Na+ and Cl−) and minimum repulsion between similarly charged ions (e.g., Na+ and Na+, or Cl− and Cl−)
Ordered arrangement of oppositely charged ions in the crystal lattice. When stress is applied, ions of the same charge are brought close together. Repulsion between like charges occur, which results in fracture (cleavage) of the crystal lattice
When a solute dissolves in a solvent, the energy released from forming solute-solvent interactions must be sufficient to compensate for the energy needed to break up the attractive forces between solvent particles as well as those between the solute particles
Solubility of ionic compounds in polar solvents (e.g. water)
The giant ionic lattice is broken up. The cations and anions form ion-dipole attractions with the solvent molecules (water). Energy is released as a result of these interactions
Not all ionic compounds are soluble in water. Lattice energy in such compounds is so exothermic (compared to ion-dipole attractions) that the hydration energy of the ions is insufficient to overcome the strong ionic bonds holding the ions in their lattice (e.g. MgO, PbCl2)
Solubility of ionic compounds in non-polar / organic solvents
The energy released from forming ion-solvent attractions is insufficient to compensate for the energy required to break up the relatively stronger ionic bonds in the lattice
Lattice energy in ionic compounds can be so exothermic (compared to ion-dipole attractions) that the hydration energy of the ions is insufficient to overcome the strong ionic bonds holding the ions in their lattice (e.g. MgO, PbCl2)
Solid Cu has a giant metallic structure, which consists of a lattice of copper cations surrounded by a sea of delocalised electrons with strong metallic bonds holding them together
Large amount of energy needed to overcome the strong electrostatic forces of attraction between the positively charged cations and the mobile 'sea' of delocalised electrons (metallic bond) in the metallic lattice