(G S Manku, email: manku.gs@gmail.com)
A solution is a homogeneous mixture of two or more chemical substances at the molecular level. The composition of a solution of solutions may vary within certain limits and may be regarded as a molecular dispersion of substances within each other.
The chemical component present in smaller amounts is regarded as solute and the component present in larger amounts is termed as solvent. The terms solute and solvent are interchangeable. In a 15 % acetone – 85 % water mixture, acetone is solute present in water as solvent, whereas in 85 % acetone – 15 % water mixture, water becomes the solute present in acetone as solvent.
Generally, there is a limit to solubility of solutes in a solvent called the solubility of the solute. When a small amount of solute is added to a solvent, on stirring, it gives a clear solution. Once the limit is reached, addition of further solute will lead to a state where there is equilibrium between undissolved solute and dissolved solute. The solution is such a state is called a saturated solution.
A solution having water as solvent is called an aqueous solution. This may have ionic species derived from the solute, or covalent molecules dissolved with (carbon dioxide, ammonia, ethanol, acetone, hydrogen cyanide, etc.) or with partial or almost complete ionization (hydrogen chloride, hydrogen fluoride, nitric acid, acetic acid, etc.).
The different solutes have a wide range of solubility, for which, presently, a foolproof explanation is npt available.
The dissolution of a solute in a solvent is analogous to melting process. In the melting process, the thermal and vibration energy of the constituent particles (ions or molecules) of the solid, arranged in a particular lattice structure, exceeds their lattice energy. This results in free movement of the particles, the lattice breaks and the solid melts. Similarly, in the dissolution process, the solvent molecules attract the constituent particles of the solid, generally through ion–dipole or dipole–dipole attractions. This results in weakening of the interlattice forces. As the interlattice forces weaken, the constituent particles of the solute spread around in the solvent (where they can move freely). A solution is formed.
In general, solutes with high melting point (having high lattice energy) have a low solubility.
It is therefore expected that the solubility of the solutes will increase with increase in temperature. Different types of forces are involved in the dissolution process.
The term solvation energy includes both the all the different types of energies.
The plots of solubility of a solute in a solvent at different temperatures are called the solubility curves of the solutes. Three types of solubility curves are observed.
Figure 11.1.1 Solubility curves of (a) sodium sulphate,
(b) potassium nitrate and (c) sodium chloride
When an ionic solute is placed in water, ion–dipole interactions take place and the water molecules align along the surface of the solid. Their negatively charged oxygen ends are towards the cations and the positively charged hydronium (proton) ends are towards the anions. Due to the electrostatic attractions between the opposite charges at the surface, the inter-ionic attractions in the solid lattice are weakened. Some of the surface ions get pulled away by the solvent (due to the thermal vibration energies) as hydrated ions and form a solution. Generally, ionic solutes have a greater solubility in the solvent with higher dielectric constants.
There is a strong hydrogen bonding in water. In order to be soluble in water, the solute must weaken these hydrogen bonds. The extent to which the solute can weaken the hydrogen bonds present in water and form stronger ion –dipole bonds, determines the solubility in water.
The nonpolar solutes are not able to break the hydrogen bonding in water as they cannot form strong bonds with water molecules and get ‘squeezed out’, i.e., they do not go into solution to any appreciable limit.
This is true of other hydrogen bonded solvents also.
Long-chain aliphatic alcohols, amines or carboxylates have a nonpolar hydrophobic carbon chain and a polar end which can form strong hydrogen bonding water. When these compounds are placed in water, they are swept to the surface in such a way that their polar ends are in water and the nonpolar ends are above the surface (Figure 11.1.2). In this way, a uni-molecular film is obtained on the surface.
Figure 11.1.2 Pictorial representation of dissolution of
polar ends of long-chain forming uni-molecular layer
of the solid above the surface of water.
Such solids find application in covering the liquid surface with unimolecular layers
Like dissolves like is a familiar rule applicable to the solubility of the solutes with respect to chemical structure and dipole nature of solvent. Thus, paraffins dissolve readily in benzene – both are hydrocarbons but polyhydric sugars are water soluble and insoluble in benzene.
Though rigid rules regarding solubility of the solutes in terms of size, charge and electronic structure of ions and compounds cannot be framed, some generalizations can, however be made.
In solution of paraffins (alkanes) in petrol, the solute retains its molecular character, whereas dissolution of say, zinc fluoride in hydrochloric acid, is clearly due to a chemical reaction:
ZnF2 + 2HCl → ZnCl2 + 2HF
Between these two extremes of solution, dissolution of solutes may involve gradual transition from physical to chemical process without a clear-cut demarcation.
Dissolution of sodium chloride in water is clearly a physical process as crystallization of the solution obtained gives the original solute. Dissolution of sodium chloride in water is clearly a physical process as crystallization of the solution obtained gives the original solute. Dissolution of anhydrous sodium carbonate in water or copper sulphate in dilute sulphuric acid gives a clear solution, which upon crystallization, gives the hydrated salts of original solutes (Na2CO3.10H2O or CuSO4.5H2O). However, these processes do not involve any chemical change in the properties of the solute and are also regarded as a normal solution formation.
However, dissolution of metals in acids or alkalis, of solutes in sulphuric acid, etc. generally involve chemical reactions. Chemical reactions which help dissolution may be of acid–base or redox reactions:
Na2O + H2O → 2NaOH (Solution of Na2O in water)
Na2O + H2O → 2Na+ + OH – (Solution of Na2O in water)
Al(OH)3 + 3HCl → Al3+ + 3Cl– + 3H2O
(Solution of Al(OH)3 in alkali)
Zn(OH)2 + 2OH– → ZnO22– + 3H2O (Solution of Zn(OH)3 in alkali)
Zn(OH)2 + 2HCl → Zn2+ + 2Cl– + 2H2O
(Solution of Zn(OH)2 in acids)
Ca3(PO4)2 + 6H+ → 3Ca2+ + 2H3PO4
(Solution of Ca(PO4)3 in acids)
2Al + 2H2O + 2OH– → 2AlO2– + 3H2 (Solution of Al in alkali)
3HgS + 2NO3– + 8H+ → 3Hg2+ + 3S + 2NO + 4H2O
(Solution of HgS in HNO3)
These processes cannot be classified as dissolution as upon crystallization of the solution obtained by evaporation, original solute cannot be recovered.
The difference between the solutions of nonpolar solutes in nonpolar solvents and mixing of ideal gases chiefly due to weak solute–solvent and solute–solvent interactions. In these cases, the free energy change ΔG for the dissolution will be due to the entropy changes (ΔS) only
ΔG = ΔH – TΔS = – TΔS (as ΔH = 0)
As for ideal gases, for mixing, if x1 and x2 are the mole fractions of the solute and solvent,
ΔS = – R(x1 ln x1 + x2 ln x2)
And, ΔG = – RT(x1 ln x1 + x2 ln x2)
At 298 K, the free energy of mixing is small, maximum value of free energy mixing released [being at δ(ΔG/ δ (x1) = 0] is at x1 = 0.5, and is – 2 8.314 298 0.5 log 0.5 = 172 J mol –1 or 1.72 kJ mol–1 only.
Many solutes dissolve in solvents due to complex formation. Examples of solvent extraction of metal complexes into organic solvents demonstrate this phenomenon. Most familiar is the extraction of nickel(II) into dimethylglyoxime (HDMG) solutions of chloroform:
Ni2+ + 2(H DMG) → [Ni(DMG)2] + 2H+
Even in aqueous solutions, many substances dissolve due to complex formation:
SnC2O4 + C2O42–⇌ [Sn(C2O4)2]2–
AgCl + Cl– ⇌ [AgCl2] –
CuCl + 2KCN ⇌ [Cu(CN)2] – + 2K+ + Cl–
Cr(OH)3 + 3OH– ⇌ [Cr(OH)6]3-
CaHPO4 + H2Y2– ⇌ [CaY]2– + H3PO4 (Y = EDTA)
In these cases also, the original solute does not get crystallized out from the solutions obtained.
The dissolution of the solute can be considered in terms of a Born – Haber cycle. The overall enthalpy of solution, ΔHsoln is the sum of the enthalpy of dissociation of the solid into gaseous ions by giving lattice energy U to the system and enthalpy of dissolution of the gaseous ions releasing the hydration enthalpy of the solution ΔHsolv:
M+A–(s) → M(g)+ + A(g)– ΔH = – U
M(g)+ + A(g)– + solvent → M(solv)+ + A(solv) – ΔH = ΔHsolv
Adding. M+A – + solv → M(solv)+ + A(solv) – ΔHsoln = – U + ΔHsolv
ΔHsoln depends on
The lattice energy depends upon the type and size of the ions. The ion–ion interactions are definitely stronger than ion–dipole interactions, and are comparable to the lattice energy. Hence, ΔHsoln is a delicate balance of lattice energy and the solvation energy of ions, and can be either positive or negative. If ΔHsoln is positive, cooling occurs during dissolution. But if ΔHsoln term is highly positive, the entropy changes (T ΔS term) may not be sufficiently high to make the dissolution spontaneous. The compound becomes insoluble, e.g. CaF2, Al2O3, Ca3(PO4)2, ZnS, etc. (in these cases, ΔHsoln = – RT ln KSP is a small difference between two large terms U and ΔHsoln.)
Please note that both water soluble as well as water insoluble salts have large hydration energy (CaI2 = – 2.14 MJ mol –1, CaF2 = – 6.78 MJ mol –1) as well as small hydration energy (KI = – 610 kJ mol –1, LiF = – – 1003 kJ mol –1). Hence, the hydration energy (ΔHsoln) alone does not determine the solubility of compounds; Lattice energy (U) must also be considered for predicting solubilities. Both U and ΔHsoln depend upon the sizes and charges on the ions. Since U is inversely proportional to the sum of the ionic radii of cation (rc) and anion (ra), whereas ΔHsoln is sum of two terms each inversely proportional to the radius of the ion,
U = f1 / (rc + ra)
ΔHsoln = f2 / rc + f3 / ra
In actual practice, lattice energy is higher than solvation energy for similar sized ions and gets reduced if the size of one of the ions becomes very large. The solvation energy, on the other hand is the sum of two terms. If one of these terms is very large due to very small size of the ion, the total sum may still be large enough despite the large size of the other ion. This is shown by solubility of alkali metal halides. CsI is least soluble alkali metal iodide and LiF is least soluble alkali metal fluoride and lithium halide.
It is observed that the solubilitiy of alkali metal halides increase with increase in difference between the hydration energies of the constituent ions.
Large sized metal ion complexes can be isolated in solid state only by using an equally large counter ion. Thus, though [Ni(CN)5]3 – exists in solution, crystallization of potassium salt gives only K2[NiCN)4].H2O; however, the large sized anion can be crystallized as the [Cr(en)3][Ni(CN)5].1.5H2O salt.
In nonpolar solvents, solvation energies of the ions are considerable low due to weak ion–induced dipole interactions. Hence, the lattice energy becomes higher than the solvation energy and the ions salts are generally insoluble in nonpolar solvents.
The insolubility of nonpolar solutes in polar solvents cannot be explained so obviously. The solute–solvent interactions are weak dipole – induced dipole interactions, and should be stronger than London’s forces which hold nonpolar solutes in solid state. Entropy of mixing is always favorable for dissolution. It appears that both these types of favorable factors are offset by loss of the energy from breaking of the hydrogen bonding in solvents.