9. Solutions
Francois-Marie Raoult was a French chemist who conducted research into the behaviour of solutions, especially their physical properties.
In his first research paper, he described the action of solutes in depressing the freezing point of the solutions. He also gave a relation between the vapour pressure of the solution with the molecular weight of the solute.
Learning Objectives
After studying this unit students will be able to
- describe the formation of different types of solutions
- express the concentration of a solution in different units
- prepare solutions of required concentrations by diluting the stock solution
- state Henry’s and Raoult’s Law
- explain the deviation of real solutions from Raoult’s Law
- correlate colligative properties of solutions with the molar masses of their solutes
- explain the abnormal colligative properties
- define Van’t Hoff factor and calculate degree of dissociation / association
9.1 INTRODUCTION
There are many chemicals that play an important role in our daily life. All these chemicals are in different physical forms, viz solid, liquid and gas. If we do close examination on their composition, we could find that most of them are mixtures and rarely pure substances. One more interesting aspect is that most of the mixtures are homogeneous irrespective of their physical state and such homogeneous mixtures are called as solutions.
Sea water is one of the naturally existing solutions which covers more than \( 70\% \) of the earth’s surface. We cannot imagine life on earth without sea water. It contains many dissolved solids, mostly NaCl. Another important naturally occurring solution is air. Air is a homogeneous mixture of nitrogen, oxygen, carbon dioxide, and other trace gases. Even solid material such as brass is a homogeneous mixture of copper and zinc.
In the above examples the solutions are in different physical states viz. liquid (sea water), gas (air) and solid (alloys), and one common property of all the above is their homogeneity. The homogeneity implies uniform distribution of their constituents or components throughout the mixture. In this chapter, we learn about the solutions and their properties.
9.2 Types of solutions
A solution is a homogeneous mixture of two or more substances, consisting of atoms, ions or molecules. The compound that is present in largest amount in a homogeneous mixture is called the solvent, and others are solutes. For example, when a small amount of NaCl is dissolved in water, a homogeneous solution is obtained. In this solution, \( \mathrm{Na^{+}} \) and \( \mathrm{Cl^{-}} \) ions are uniformly distributed in water. Here water is the solvent as the amount of water is more compared to the amount of NaCl present in this solution, and NaCl is the solute.
The commonly used solutions are the solutions in which a solid solute is dissolved in a liquid solvent. However, solute or solvent can be in any of the three states of matter (solid, liquid, gas). If water is used as the solvent, the resultant solution is called as an aqueous solution. If solvents (Benzene, \( \mathrm{CCl_4} \), ether etc.) other than water is used, then the resultant solution is called as a nonaqueous solution.
The following table illustrates the different types of solutions based on the physical state of the solute and solvent.
Table 9.1 Types and examples of solutions
| S. No. | State of solution | Solution | Solvent | Examples |
|---|---|---|---|---|
| 1 | Gaseous solution | Gas | Gas | Air (A mixture of nitrogen, oxygen and other gases) |
| Liquid | Gas | Humid oxygen (Oxygen containing water) | ||
| 2 | Liquid solutions | Solid | Gas | Camphor in nitrogen gas |
| Gas | Liquid | \( \mathrm{CO_2} \) dissolved in water (carbonated water) | ||
| Liquid | Liquid | Ethanol dissolved in water | ||
| Solid | Liquid | Salt water | ||
| 3 | Solid solutions | Gas | Solid | Solution of \( \mathrm{H_2} \) in palladium |
| Liquid | Solid | Amalgam of potassium (used for dental filling) | ||
| Solid | Solid | Gold alloy (of copper used in making Jewelery) |
9.3 Expressing concentration of solutions
In our life we have come across many solutions of varying strengths or concentrations. The concentration of a solution is defined as the amount of solute present in a given amount (mass or volume) of solution or solvent. The concentration of a solution can be expressed in different ways as listed below.
Table 9.2 Different concentration terms with expressions and illustrations
| S. No. | Concentration term | Expression | Illustration |
|---|---|---|---|
| 1 | Molarity (M) | \( \frac{\text{Number of moles of solute}}{\text{Volume of solution in L}} \) | 5.85 g of sodium chloride is dissolved in water and the solution was made up to 500 mL using a standard flask. The strength of the solution in molarity is \( \frac{5.85}{58.5 \times 0.5 \mathrm{L}} = 0.2 \mathrm{M} \) |
| 2 | Molality (m) | \( \frac{\text{Number of moles of solute}}{\text{Mass of solvent in kg}} \) | 5.85 g of NaCl is dissolved in 500 g of water. The strength of the solution in molality is \( \frac{5.85}{58.5 \times 0.5 \mathrm{kg}} = 0.2 \mathrm{m} \) |
| 3 | Normality (N) | \( \frac{\text{Number of gram equivalents of solute}}{\text{Volume of solution in L}} \) | 3.65 g of HCl is dissolved in water and the solution was made up to 500 mL. The strength of the solution in normality is \( \frac{3.65}{36.5 \times 0.5 \mathrm{L}} = 0.2 \mathrm{N} \) |
| 4 | Formality (F) | \( \frac{\text{Number of formula mass of solute}}{\text{Volume of solution in L}} \) | 5.85 g of sodium chloride is dissolved in water and the solution was made up to 500 mL using a standard flask. The strength of the solution in formality is \( \frac{5.85}{58.5 \times 0.5 \mathrm{L}} = 0.2 \mathrm{F} \) |
| 5 | Mole fraction (of a component) (x) | \( \frac{\text{Number of moles of the component}}{\text{Total number of moles of all the components present in solution}} \) | Consider a solution containing two components A and B whose mole fractions are \( x_A \) and \( x_B \), respectively. Let the number of moles of the two components A and B be \( n_A \) and \( n_B \), respectively. \( x_A = \frac{n_A}{n_A + n_B} \) and \( x_B = \frac{n_B}{n_A + n_B} \). Now, \( x_A + x_B = \frac{n_A}{n_A + n_B} + \frac{n_B}{n_A + n_B} = 1 \). 0.5 mole of ethanol is mixed with 1.5 moles of water. The mole fraction of ethanol in the above solution is \( \frac{0.5}{0.5 + 1.5} = \frac{0.5}{2.0} = 0.25 \). The mole fraction of water in the above solution is \( \frac{1.5}{2.0} = 0.75 \). |
| 6 | Mass percentage (% w/w) | \( \frac{\text{Mass of the solute (in g)}}{\text{Mass of solution (in g)}} \times 100 \) | Neomycin, aminoglycoside antibiotic cream contains 300 mg of neomycin sulphate the active ingredient, in 30 g of ointment base. The mass percentage of neomycin is \( \frac{0.3 \mathrm{g}}{30 \mathrm{g}} \times 100 = 1\% \ \mathrm{w/w} \) |
Evaluate Yourself
If 5.6 g of KOH is present in (a) 500 mL and (b) 1 litre of solution, calculate the molarity of each of these solutions.
2.82 g of glucose is dissolved in 30 g of water. Calculate the mole fraction of glucose and water.
The antiseptic solution of iodopovidone for the use of external application contains 10% w/v of iodopovidone. Calculate the amount of iodopovidone present in a typical dose of 1.5 mL.
A litre of sea water weighing about 1.05 kg contains 5 mg of dissolved oxygen \( (\mathrm{O}_{2}) \). Express the concentration of dissolved oxygen in ppm.
The concentration of a solution is expressed in different units. The choice of unit depends on the type of measurement applied. For example, in complexometric titrations involving EDTA, the concentration of solution is expressed in formality because EDTA exists as \( \mathrm{H_4Y} \). In the case of redox titration involving \( \mathrm{KMnO_4} \) vs \( \mathrm{FeSO_4} \), the strength of \( \mathrm{KMnO_4} \) is expressed in normality. Similarly, for the osmotic pressure measurement, we use the molarity of the solution. Hence, we need to learn to convert one concentration unit into another, which we will practice at the end of this chapter.
9.3.1 Dilution of solution
The concentration of a solution can be reduced by adding more solvent. This process is called dilution. In the initial solution, the number of moles of solute is \( \mathrm{M_1V_1} \) and in the final solution after dilution it becomes \( \mathrm{M_2V_2} \). Since the number of moles of solute taken remains constant after dilution, we can write
\[ \mathrm{M_1V_1 = M_2V_2} \qquad (9.1) \]Similarly, for dilution in terms of normality,
\[ \mathrm{N_1V_1 = N_2V_2} \qquad (9.2) \]This relation is used to prepare a less concentrated solution from a more concentrated solution.
The concentration of the solution can be expressed in different units. The choice of unit depends on the requirement. For example, we express the strength of EDTA as formality because of its complex formula. For redox reactions, we use normality. In some cases, we need to convert one concentration unit to another.
9.3.2 Advantages of using standard solutions
- The error in weighing the solute can be minimised by using concentrated stock solution that requires large quantity of solute.
- We can prepare working standards of different concentrations by diluting the stock solution, which is more efficient since consistency is maintained.
- Some of the concentrated solutions are more stable and are less likely to support microbial growth than working standards used in the experiments.
Example Problem 1
What volume of 4M HCl and 2M HCl should be mixed to get \( 500 \ \mathrm{mL} \) of \( 2.5 \ \mathrm{M} \) HCl?
Let the volume of 4M HCl required to prepare \( 500 \ \mathrm{mL} \) of \( 2.5 \ \mathrm{M} \) HCl = \( \mathrm{x \ mL} \)
Therefore, the required volume of 2M HCl = \( (500 - x) \ \mathrm{mL} \)
We know from the equation (9.1)
\[ \mathrm{C_1V_1 + C_2V_2 = C_3V_3} \]\[ \mathrm{(4x) + 2(500 - x) = 2.5 \times 500} \]\[ \mathrm{4x + 1000 - 2x = 1250} \]\[ \mathrm{2x = 1250 - 1000} \]\[ \mathrm{x = \frac{250}{2} = 125 \ mL} \]Evaluate Yourself
Describe how would you prepare the following solution from pure solute and solvent (a) 1 L of aqueous solution of 1.5 M \( \mathrm{CoCl_2} \). (b) \( 500 \ \mathrm{mL} \) of \( 6.0\% \) (V/V) aqueous methanol solution.
How much volume of 6 M solution of NaOH is required to prepare \( 500 \ \mathrm{mL} \) of 0.250 M NaOH solution.
9.4 Solubility of the solutes
Solubility of a solute is the maximum amount of solute that can be dissolved in a specific amount of solvent at a specified temperature. When maximum amount of solute is dissolved in a solvent, any more addition of solute will result in precipitation at a given temperature and pressure. Such a solution is called as a saturated solution. The solubility of a substance at a given temperature is defined as the amount of the solute that can be dissolved in \( 100 \ \mathrm{g} \) of the solvent at a given temperature to form a saturated solution.
9.4.1 Factors influencing the solubility
The solubility of a solute generally depends on the nature of the solute and the solvent in which it is dissolved. It also depends on the temperature and pressure of the solution.
Nature of solute and solvent
Sodium chloride, an ionic compound, dissolves readily in a polar solvent such as water, but it does not dissolve in non-polar organic solvents such as benzene or toluene. Many organic compounds dissolve readily in organic solvents and do not dissolve in water. Different gases dissolve in water to different extents: for example, ammonia is more soluble than oxygen in water.
Effect of temperature
Solid solute in liquid solvent
Generally, the solubility of a solid solute in a liquid solvent increases with increase in temperature. When the temperature is increased, the average kinetic energy of the molecules of the solute and the solvent increases. The increase in kinetic energy facilitates the solvent molecules to break the intermolecular attractive forces that keep the solute molecules together and hence the solubility increases.
When a solid is added to a solvent, it begins to dissolve. i.e. the solute leaves from the solid state (dissolution). After some time, some of the dissolved solute returns back to the solid state (recrystallisation). If there is excess of solid present, the rate of both these processes becomes equal at a particular stage. At this stage an equilibrium is established between the solid solute molecules and dissolved solute molecules.
\[ \text{Solute (solid)} \rightleftharpoons \text{Solute (dissolved)} \]According to Le-Chatelier principle, if the dissolution process is endothermic, the increase in temperature will shift the equilibrium towards right i.e solubility increases. For an exothermic reaction, the increase in temperature decreases the solubility. The solubilities of ammonium nitrate, calcium chloride, ceric sulphate nano-hydrate and sodium chloride in water at different temperatures are given in the following graph.
The following conclusions are drawn from the above graph.
- The solubility of sodium chloride does not vary appreciable as the maximum solubility is achieved at normal temperature. In fact, there is only \( 10\% \) increase in solubility between \( 0^{\circ} \) to \( 100^{\circ} \) C.
- The dissolution process of ammonium nitrate is endothermic, the solubility increases steeply with increase in temperature.
- In the case of ceric sulphate, the dissolution is exothermic and the solubility decreases with increase in temperature.
- Even though the dissolution of calcium chloride is exothermic, the solubility increases moderately with increase in temperature. Here, the entropy factor also plays a significant role in deciding the position of the equilibrium.
Gaseous solute in liquid solvent
In the case of gaseous solute in liquid solvent, the solubility decreases with increase in temperature. When a gaseous solute dissolves in a liquid solvent, its molecules interact with solvent molecules with weak intermolecular forces. When the temperature increases, the average kinetic energy of the molecules present in the solution also increases. The increase in kinetic energy breaks the weak intermolecular forces between the gaseous solute and liquid solvent which results in the release of the dissolved gas molecules to the gaseous state. Moreover, the dissolution of most of the gases in liquid solvents is an exothermic process, and in such processes, the increase in temperature decreases the dissolution of gaseous molecules.
Activity
Open the soda bottle and put a balloon over it. The balloon will inflate with the released carbon dioxide from the soda. Carry out the same experiment by placing the soda bottle in a container of hot water. You will observe the balloon is inflated much faster now. This shows the decrease in solubility of gases in solution with increase in temperature. In the rivers where hot water is discharged from industrial plants, the aquatic lives are less sustained due to the decreased availability of dissolved oxygen.
Effect of pressure
Generally the change in pressure does not have any significant effect in the solubility of solids and liquids as they are not compressible. However, the solubility of gases generally increases with increase of pressure.
Consider a saturated solution of a gaseous solute dissolved in a liquid solvent in a closed container. In such a system, the following equilibrium exists.
\[ \text{Gas (in gaseous state)} \rightleftharpoons \text{Gas (in solution)} \]According to Le-Chatelier principle, the increase in pressure will shift the equilibrium in the direction which will reduce the pressure. Therefore, more number of gaseous molecules dissolves in the solvent and the solubility increases.
9.5 Henry’s law
William Henry investigated the relationship between pressure and solubility of a gaseous solute in a particular solvent. According to him, “the partial pressure of the gas in vapour phase (vapour pressure of the solute) is directly proportional to the mole fraction (x) of the gaseous solute in the solution at low concentrations”. This statement is known as Henry’s law.
Henry’s law can be expressed as,
\[ \mathrm{P_{solute} \propto x_{solute \ in \ solution}} \]\[ \mathrm{P_{solute} = K_H x_{solute \ in \ solution}} \]Here, \( \mathrm{P_{solute}} \) represents the partial pressure of the gas in vapour state which is commonly called as vapour pressure. \( \mathbf{x}_{\mathrm{solute}} \) in solution represents the mole fraction of solute in the solution. \( \mathrm{K}_{\mathrm{H}} \) is an empirical constant with the dimensions of pressure. The value of \( \mathrm{K}_{\mathrm{H}} \) depends on the nature of the gaseous solute and solvent. The above equation is a straight-line in the form of \( \mathrm{y = mx} \). The plot of partial pressure of the gas against its mole fraction in a solution will give a straight line as shown in fig 9.3. The slope of the straight line gives the value of \( \mathrm{K}_{\mathrm{H}} \).
Why the carbonated drinks are stored in a pressurized container?
We all know that the carbonated beverages contain carbon dioxide dissolved in them. To dissolve the carbon dioxide in these drinks, the \( \mathrm{CO}_{2} \) gas is bubbled through them under high pressure. These containers are sealed to maintain the pressure. When we open these containers at atmospheric pressure, the pressure of the \( \mathrm{CO}_{2} \) drops to the atmospheric level and hence bubbles of \( \mathrm{CO}_{2} \) rapidly escape from the solution and show effervescence. The burst of bubbles is even more noticeable, if the soda bottle is in warm condition.
Why deep-sea divers use air diluted with helium gas in their air tanks?
The professional deep-sea divers carry a compressed air tank for breathing at high pressure under water. The normal compressed air contains nitrogen and oxygen and these gases are not very soluble in blood and other body fluids at normal pressure. As the pressure at that depth is far greater than the surface atmospheric pressure, more nitrogen dissolves in the blood and other body fluids when the diver breathes from tank. When the diver ascends to the surface, the pressure decreases, the dissolved nitrogen comes out of the blood and other body fluids quickly forming bubbles in the blood stream. These bubbles restrict blood flow, affect the transmission of nerve impulses and can even burst the capillaries or block them. This condition is called “the bends”, which are painful and dangerous to life. Nowadays, to avoid such dangerous condition, the professional divers, use air diluted with helium gas (about 11.7% Helium, 56.2% Nitrogen and 32.1% Oxygen), because of lower solubility of helium in the blood than nitrogen. Moreover, because of small size of helium atoms they can pass through cell walls without damaging them. The excess oxygen dissolved in the blood is used in metabolism and does not cause the condition of bends.
9.5.1 Limitations of Henry’s law
- Henry’s law is applicable at moderate temperature and pressure only.
- Only the less soluble gases obeys Henry’s law
- The gases reacting with the solvent do not obey Henry’s law. For example, ammonia or HCl reacts with water and hence does not obey this law. \[ \mathrm{NH_3 + H_2O \rightleftharpoons NH_4^+ + OH^-} \]
- The gases obeying Henry’s law should not associate or dissociate while dissolving in the solvent.
Example Problem 2
0.24 g of a gas dissolves in 1 L of water at 1.5 atm pressure. Calculate the amount of dissolved gas when the pressure is raised to 6.0 atm at constant temperature.
\[ \mathrm{p_{solute} = K_H x_{solute \ in \ solution}} \]At pressure 1.5 atm,
\[ \mathrm{P_1 = K_H x_1} \qquad (1) \]At pressure 6.0 atm,
\[ \mathrm{P_2 = K_H x_2} \qquad (2) \]Dividing equation (1) by (2)
From equation \( \mathrm{P_1 / P_2 = x_1 / x_2} \)
\[ 1.5 / 6.0 = 0.24 / x_2 \]Therefore \( \mathrm{x_2} = \frac{0.24 \times 6.0}{1.5} = 0.96 \ \mathrm{g / L} \)
Evaluate Yourself
Calculate the proportion of \( \mathrm{O}_{2} \) and \( \mathrm{N}_{2} \) dissolved in water at \( 298 \ \mathrm{K} \). When air containing \( 20\% \ \mathrm{O}_{2} \) and \( 80\% \ \mathrm{N}_{2} \) by volume is in equilibrium with water at 1 atm pressure. Henry’s law constants for two gases are \( \mathrm{K_{H}(O_{2}) = 4.6 \times 10^{4}} \) atm and \( \mathrm{K_{H}(N_{2}) = 8.5 \times 10^{4}} \) atm.
Explain why the aquatic species are more comfortable in cold water during winter season rather than warm water during the summer.
9.6 Vapour pressure of liquid
Generally, liquids have a tendency to evaporate. If the kinetic energy of molecules in the liquid state overcomes the intermolecular force of attraction between them, then the molecules will escape from the liquid state. This process is called ’evaporation’ and it happens on the surface of the liquid.
If evaporation is carried out in a closed container then the vapour remains in contact with the surface of the liquid. These vapour molecules are in continuous random motion during which they collide with each other and also with the walls of the container. As the collision is inelastic, they lose their energy and as result the vapour returns back to liquid state. This process is called as ‘condensation’.
Evaporation and condensation are continuous processes. If the process is carried out in a closed system, a stage is reached when the rate of evaporation becomes equal to the rate of condensation. Thus, an equilibrium is established between liquid and its vapour. The pressure of the vapour in equilibrium with its liquid is called vapour pressure of the liquid at the given temperature. The vapour pressure of a liquid depends on its nature, temperature and the surface area. The following simple apparatus demonstrates the measurement of vapour pressure of a liquid.
9.7 Vapour pressure of liquid solutions
When a solute (of any physical state - solid, liquid or gas) is dissolved in a liquid solvent the resultant solution is called a liquid solution. The solution which contains only two components (one solvent and one solute) is called a binary solution. We have already discussed the solution of a gaseous solute in liquid solvent under Henry’s law.
9.7.1 Vapour pressure of binary solution of liquid in liquids
Now, let us consider a binary liquid solution formed by dissolving a liquid solute ‘A’ in a pure solvent ‘B’ in a closed vessel. Both the components A and B present in the solution would evaporate and an equilibrium will be established between the liquid and vapour phases of the components A and B.
The French chemist Raoult, proposed a quantitative relationship between the partial pressures and the mole fractions of two components A & B, which is known as Raoult’s Law. This law states that “in the case of a solution of volatile liquids, the partial vapour pressure of each component (A & B) of the solution is directly proportional to its mole fraction”.
According to Raoult’s law,
\[ \mathrm{P_A \propto x_A} \qquad (9.3) \]\[ \mathrm{P_A = k x_A} \]when \( \mathbf{x_A} = 1 \), \( \mathrm{k = p_A^{\circ}} \)
where \( \mathrm{p_A^{\circ}} \) is the vapour pressure of pure component ‘A’ at the same temperature.
Therefore,
\[ \mathrm{P_A = p_A^{\circ} x_A} \qquad (9.4) \]Similarly, for component ‘B’
\[ \mathrm{P_B = p_B^{\circ} x_B} \qquad (9.5) \]\( \mathbf{x_A} \) and \( \mathbf{x_B} \) are the mole fraction of the components A and B respectively.
According to Dalton’s law of partial pressure the total pressure in a closed vessel will be equal to the sum of the partial pressures of the individual components.
Hence,
\[ \mathrm{P_{total} = P_A + P_B} \qquad (9.6) \]Substituting the values of \( \mathrm{p_A} \) and \( \mathrm{p_B} \) from equations (9.4) and (9.5) in the above equation,
\[ \mathrm{P_{total} = x_A p_A^{\circ} + x_B p_B^{\circ}} \qquad (9.7) \]We know that \( \mathrm{x_A + x_B = 1} \) or \( \mathrm{x_A = 1 - x_B} \)
Therefore,
\[ \mathrm{P_{total} = (1 - x_B) p_A^{\circ} + x_B p_B^{\circ}} \qquad (9.8) \]\[ \mathrm{P_{total} = p_A^{\circ} + x_B (p_B^{\circ} - p_A^{\circ})} \qquad (9.9) \]The above equation is of the straight-line equation form \( \mathrm{y = mx + c} \). The plot of \( \mathrm{P_{total}} \) versus \( \mathbf{x_B} \) will give a straight line with \( (\mathrm{p_B^{\circ} - p_A^{\circ}}) \) as slope and \( \mathrm{p_A^{\circ}} \) as the y intercept.
Let us consider the liquid solution containing toluene (solute) in benzene (solvent).
The vapour pressures of pure toluene and pure benzene are 22.3 and \( 74.7 \ \mathrm{mmHg} \), respectively. The above graph shows, the partial vapour pressure of the pure components increases linearly with the increase in the mole fraction of the respective components. The total pressure at any composition of the solute and solvent is given by the following straight line (represented as red line) equation.
\[ \mathrm{P_{solution} = P_{solute}^{\circ} + X_{benzene} (P_{benzene}^{\circ} - P_{solute}^{\circ})} \qquad (9.10) \]9.7.2 Vapour pressure of binary solution of solids in liquids
When a nonvolatile solute is dissolved in a pure solvent, the vapour pressure of the pure solvent will decrease. In such solutions, the vapour pressure of the solution will depend only on the solvent molecules as the solute is nonvolatile.
For example, when sodium chloride is added to the water, the vapour pressure of the salt solution is lowered. The vapour pressure of the solution is determined by the number of molecules of the solvent present in the surface at any time and is proportional to the mole fraction of the solvent.
Where \( x_A \) is the mole fraction of the solvent
\[ \mathrm{P_{solution} = k x_A} \qquad (9.12) \]When \( x_A = 1 \), \( \mathrm{K = P_{solvent}^{\circ}} \) (\( \mathrm{P_{solvent}^{\circ}} \) is the partial pressure of pure solvent)
\[ \mathrm{P_{solution} = P_{solvent}^{\circ} x_A} \qquad (9.13) \]\[ \frac{\mathrm{P_{solution}}}{\mathrm{P_{solvent}^{\circ}}} = x_A \qquad (9.14) \]\[ 1 - \frac{\mathrm{P_{solution}}}{\mathrm{P_{solvent}^{\circ}}} = 1 - x_A \qquad (9.15) \]\[ \frac{\mathrm{P_{solvent}^{\circ} - P_{solution}}}{\mathrm{P_{solvent}^{\circ}}} = x_B \qquad (9.16) \]Where \( x_B \) is the mole fraction of the solute (\( \because x_A + x_B = 1, x_B = 1 - x_A \)).
The above expression gives the relative lowering of vapour pressure. Based on this expression, Raoult’s Law can also be stated as “the relative lowering of vapour pressure of an ideal solution containing the nonvolatile solute is equal to the mole fraction of the solute at a given temperature”.
Comparison of Raoult’s law and Henry’s law
According to Raoult’s law, for a solution containing a nonvolatile solute
\[ \mathrm{p_{solute} = p_{solvent}^{\circ} x_{solute}} \qquad (9.17) \]According to Henry’s law:
\[ \mathrm{p_{solute} = K_H x_{solute \ in \ solution}} \qquad (9.18) \]The difference between the above two expressions is the proportionality constant \( \mathrm{p_A^{\circ}} \) (Raoults Law) and \( \mathrm{K_H} \) (Henry’s Law). Henry’s law is applicable to solution containing gaseous solute in liquid solvent, while the Raoult’s Law is applicable to nonvolatile solid solute in a liquid solvent. If the solute is non volatile then the Henry’s law constant will become equal to the vapour pressure of the pure solvent \( \mathrm{(p_A^{\circ})} \) and thus, Raoult’s law becomes a special case of Henry’s law. For very dilute solutions the solvent obeys Raoult’s law and the solute obeys Henry’s law.
9.8 Ideal and non-ideal solutions
9.8.1 Ideal Solutions
An ideal solution is a solution in which each component i.e. the solute as well as the solvent obeys the Raoult’s law over the entire range of concentration. Practically no solution is ideal over the entire range of concentration. However, when the concentration of solute is very low, the dilute solution behaves ideally. If the two components present in the solution (A and B) are identical in size, structure, and having almost similar intermolecular attractive forces between them (i.e. between A-A, B-B and B-A) then the solution tends to behave like an ideal solution.
For an ideal solution
- There is no change in the volume on mixing the two components (solute & solvents). \( (\Delta \mathrm{V_{mixing} = 0}) \)
- There is no exchange of heat when the solute is dissolved in solvent \( (\Delta \mathrm{H_{mixing} = 0}) \)
- Escaping tendency of the solute and the solvent present in it should be same as in pure liquids.
Examples for ideal solutions: (Benzene & Toluene); (n-hexane & n-heptane); (Ethyl bromide & Ethyl iodide); (Chlorobenzene & Bromobenzene).
9.8.2 Non-ideal solutions
The solutions which do not obey Raoult’s law over the entire range of concentration, are called non-ideal solutions. For a non-ideal solution, there is a change in the volume and enthalpy upon mixing. i.e. \( \Delta \mathrm{H_{mixing} \neq 0} \) and \( \Delta \mathrm{V_{mixing} \neq 0} \). The deviation of the non-ideal solutions from the Raoult’s law can either be positive or negative.
Non-ideal solutions - positive deviation from Raoult’s Law
The nature of the deviation from the Raoult’s law can be explained in terms of the intermolecular interactions between solute (B) and solvent (A). Consider a case in which the intermolecular attractive forces between A and B are weaker than those between the molecules of A (A-A) and molecules of B (B-B). The molecules present in such a solution have a greater tendency to escape from the solution when compared to the ideal solution formed by A and B, in which the intermolecular attractive forces (A-A, B-B, A-B) are almost similar. Consequently, the vapour pressure of such non-ideal solution increases and it is greater than the sum of the vapour pressure of A and B as predicted by the Raoult’s law. This type of deviation is called positive deviation.
\[ \mathrm{P_A > P_A^{\circ} x_A \ and \ P_B > P_B^{\circ} x_B} \]\[ \mathrm{P_{total} > P_A^{\circ} x_A + P_B^{\circ} x_B} \qquad (9.19) \]Let us understand the positive deviation by considering a solution of ethyl alcohol and water. In this solution the hydrogen bonding interaction between ethanol and water is weaker than those hydrogen bonding interactions amongst themselves (ethyl alcohol-ethyl alcohol and water-water interactions). This results in the increased evaporation of both components (H₂O and \( \mathrm{C_2H_5OH} \)) from the aqueous solution of ethanol. Consequently, the vapour pressure of the solution is greater than the vapour pressure predicted by Raoult’s law. Here, the mixing process is endothermic i.e. \( \Delta \mathrm{H_{mixing} > 0} \) and there will be a slight increase in volume \( (\Delta \mathrm{V_{mixing} > 0}) \).
Examples for non-ideal solutions showing positive deviations: Ethyl alcohol & cyclohexane, Benzene & acetone, Carbon tetrachloride & chloroform, Acetone & ethyl alcohol, Ethyl alcohol & water.
Non-ideal solutions - negative deviation from Raoult’s Law
Let us consider a case where the attractive forces between solute (A) and solvent (B) are stronger than the intermolecular attractive forces between the individual components (A-A & B-B). Here, the escaping tendency of A and B will be lower when compared with an ideal solution formed by A and B. Hence, the vapour pressure of such solutions will be lower than the sum of the vapour pressure of A and B. This type of deviation is called negative deviation. For the negative deviation \( \mathrm{p_A < p_A^{\circ} x_A} \) and \( \mathrm{p_B < p_B^{\circ} x_B} \).
Let us consider a solution of phenol and aniline. Both phenol and aniline form hydrogen bonding interactions amongst themselves. However, when mixed with aniline, the phenol molecule forms hydrogen bonding interactions with aniline, which are stronger than the hydrogen bonds formed amongst themselves. Formation of new hydrogen bonds considerably reduce the escaping tendency of phenol and aniline from the solution. As a result, the vapour pressure of the solution is less and there is a slight decrease in volume ( \( \Delta \mathrm{V_{mixing} < 0} \) ) on mixing. During this process evolution of heat takes place i.e. \( \Delta \mathrm{H_{mixing} < 0} \) (exothermic).
9.8.3 Factors responsible for deviation from Raoult’s law
The deviation of solution from ideal behavior is attributed to the following factors.
i) Solute-solvent interactions
For an ideal solution, the interaction between the solvent molecules (A-A), the solute molecules (B-B) and between the solvent & solute molecules (A-B) are expected to be similar. If these interactions are dissimilar, then there will be a deviation from ideal behavior.
ii) Dissociation of solute
When a solute present in a solution dissociates to give its constituent ions, the resultant ions interact strongly with the solvent and cause deviation from Raoult’s law.
For example, a solution of potassium chloride in water deviates from ideal behavior because the solute dissociates to give \( \mathrm{K}^{+} \) and \( \mathrm{Cl}^{-} \) ion which form strong ion-dipole interaction with water molecules.
iii) Association of solute
Association of solute molecules can also cause deviation from ideal behaviour. For example, in solution, acetic acid exists as a dimer by forming intermolecular hydrogen bonds, and hence deviates from Raoult’s law.
iv) Temperature
An increase in temperature of the solution increases the average kinetic energy of the molecules present in the solution which causes decrease in the attractive force between them. As a result, the solution deviates from ideal behaviour.
v) Pressure
At high pressure the molecules tend to stay close to each other and therefore there will be an increase in their intermolecular attraction. Thus, a solution deviates from Raoult’s law at high pressure.
vi) Concentration
If a solution is sufficiently dilute there is no pronounced solvent-solute interaction because the number of solute molecules are very low compared to the solvent. When the concentration is increased by adding solute, the solvent-solute interaction becomes significant. This causes deviation from the Raoult’s law.
Evaluate Yourself
- Calculate the mole fractions of benzene and naphthalene in the vapour phase when an ideal liquid solution is formed by mixing \( 128 \ \mathrm{g} \) of naphthalene with \( 39 \ \mathrm{g} \) of benzene. It is given that the vapour pressure of pure benzene is \( 50.71 \ \mathrm{mmHg} \) and the vapour pressure of pure naphthalene is \( 32.06 \ \mathrm{mmHg} \) at \( 300 \ \mathrm{K} \).
9.9 Colligative properties
Pure water is tasteless. When you add sugar it becomes sweet, while addition of salt makes it salty. It implies that the properties of a solution depend on the nature of solute particles present in the solution. However, for an ideal dilute solution, the properties, namely, relative lowering of vapour pressure, elevation of boiling point, depression in freezing point and osmotic pressure do not depend on the chemical nature of the solute but depends only on the number of solute particles (ions/molecules) present in the solution. These four properties are known as colligative properties. Though the magnitude of these properties are small, they have plenty of practical applications. For example the osmotic pressure is important for some vital biological systems.
Relative lowering of vapour pressure
The vapour pressure of a solution containing a nonvolatile, non-electrolyte solute is always lower than the vapour pressure of the pure solvent. Consider a closed system in which a pure solvent is in equilibrium with its vapour. At equilibrium the molar Gibbs free energies of solvent in the liquid and gaseous phase are equal (\( \Delta G = 0 \)). When a solute is added to this solvent, the dissolution takes place and its free energy (G) decreases due to increase in entropy. In order to maintain the equilibrium, the free energy of the vapour phase must also decrease. At a given temperature, the only way to lower the free energy of the vapour is to reduce its pressure. Thus the vapour pressure of the solution must decrease to maintain the equilibrium.
We know that from the Raoult’s law the relative lowering of the vapour pressure is equal to the mole fraction of the solute (equation 9.16)
From the above equation, it is clear that the relative lowering of vapour pressure depends only on the mole fraction of the solute \( \left( \mathbf{x_B} \right) \) and is independent of its nature. Therefore, relative lowering of vapour pressure is a colligative property.
Determination of molar mass from relative lowering of vapour pressure
The measurement of relative lowering of vapour pressure can be used to determine the molar mass of a nonvolatile solute. In this method, a known mass of the solute is dissolved in a known quantity of solvent. The relative lowering of vapour pressure is measured experimentally.
According to Raoult’s law the relative lowering of vapour pressure is,
\[ \frac{\mathrm{P_{solvent}^{0} - P_{solution}}}{\mathrm{P_{solvent}^{0}}} = x_B \]Let \( \mathrm{w_A} \) and \( \mathrm{w_B} \) be the weights of the solvent and solute respectively and their corresponding molar masses are \( \mathrm{M_A} \) and \( \mathrm{M_B} \), then the mole fraction of the solute \( x_B \) is
\[ x_B = \frac{n_B}{n_A + n_B} \qquad (9.20) \]Here, \( n_A \) & \( n_B \) are the moles of the solvent and the solute respectively. For dilute solutions \( n_A >> n_B \). Hence \( n_A + n_B = n_A \). Now
\[ x_B = \frac{n_B}{n_A} \]Number of moles of solvent and the solute are,
\[ n_A = \frac{w_A}{M_A}, \quad n_B = \frac{w_B}{M_B} \]Therefore,
\[ x_B = \frac{w_B}{M_B} \times \frac{M_A}{w_A} \qquad (9.21) \]Thus,
\[ \frac{\mathrm{P_{solvent}^{0} - P_{solution}}}{\mathrm{P_{solvent}^{0}}} = \frac{w_B \times M_A}{w_A \times M_B} \]\[ \frac{\Delta P}{P_A^0} = \frac{w_B \times M_A}{w_A \times M_B} \]From the equation (9.22) the molar mass of the solute \( \mathrm{(M_B)} \) can be calculated using the known values of \( w_A \), \( w_B \), \( M_A \) and the measured relative lowering of vapour pressure.
Example Problem 3
An aqueous solution of \( 2\% \) nonvolatile solute exerts a pressure of 1.004 bar at \( 100^{\circ}C \). What is the molar mass of the solute?
\[ \frac{\Delta P}{P_A^0} = \frac{W_B \times M_A}{M_B \times W_A} \]In a \( 2\% \) solution weight of the solute is \( 2 \ \mathrm{g} \) and solvent is \( 98 \ \mathrm{g} \)
\[ \Delta P = P_A^0 - P_{solution} = 1.013 - 1.004 \ \mathrm{bar} = 0.009 \]\[ M_B = \frac{P_A^0 \times W_B \times M_A}{\Delta P \times W_A} \]\[ M_B = \frac{2 \times 18 \times 1.013}{98 \times 0.009} = 41.3 \ \mathrm{g \ mol^{-1}} \]Evaluate Yourself
- Vapour pressure of a pure liquid A is 10.0 torr at \( 27^{\circ}C \). The vapour pressure is lowered to 9.0 torr on dissolving one gram of B in \( 20 \ \mathrm{g} \) of A. If the molar mass of A is \( 200 \ \mathrm{g \ mol^{-1}} \) then calculate the molar mass of B.
Elevation of boiling point
Boiling point is an important physical property of a liquid. The boiling point of a liquid is the temperature at which its vapour pressure becomes equal to the atmospheric pressure (1 atm). When a nonvolatile solute is added to a pure solvent at its boiling point, the vapour pressure of the solution is lowered below 1 atm. To bring the vapour pressure again to 1 atm, the temperature of the solution has to be increased. As a result, the solution boils at a higher temperature \( \mathrm{T_b} \) than the boiling point of the pure solvent \( \mathrm{T_b^{\circ}} \). This increase in boiling point is known as elevation of boiling point.
The vapour pressure of the solution increases with increase in temperature as shown in the above figure. The variation of vapour pressure with respect to temperature for pure water is given by the violet coloured curve. At \( 100^{\circ}C \) the vapour pressure of water is equal to 1 atm. Hence the boiling point of water is \( 100^{\circ}C \) \( \mathrm{T_b^{\circ}} \). When a solute is added to water, the vapour pressure of the resultant solution is lowered. The variation of vapour pressure with respect to temperature for the solution is given by green curve. From the graph, it is evident the vapour pressure of the solution is equal to 1 atm pressure at the temperature \( \mathrm{T_b} \) which is greater than \( \mathrm{T_b^{\circ}} \). The difference between these two temperatures \( \mathrm{T_b} - \mathrm{T_b^{\circ}} \) gives the elevation of boiling point.
The elevation of boiling point \( (\Delta \mathrm{T_b}) = \mathrm{T_b} - \mathrm{T_b^{\circ}} \)
The elevation of boiling point is directly proportional to the concentration of the solute particles.
\[ \Delta \mathrm{T_b} \propto \mathrm{m} \qquad (9.23) \]m is the concentration of solution expressed in molality.
\[ \Delta \mathrm{T_b} = \mathrm{K_b m} \qquad (9.24) \]Where \( \mathrm{K_b} = \) molal boiling point elevation constant or Ebullioscopic constant.
If \( \mathrm{m = 1} \), then \( \Delta \mathrm{T_b} = \mathrm{K_b} \);
Hence, \( \mathrm{K_b} \) is equal to the elevation in boiling point for 1 molal solution. \( \mathrm{K_b} \) is calculated by the following expression
\[ \mathrm{K_b} = \frac{\mathrm{R T^2 M_{solvent}}}{\Delta \mathrm{H_{vaporisation}}} \]Determination of molar mass of solute from elevation of boiling point
If the solution is prepared by dissolving \( \mathrm{w_B} \ \mathrm{g} \) of solute in \( \mathrm{w_A} \ \mathrm{g} \) of solvent, then the molality is,
\[ \mathrm{m} = \frac{\text{Number of moles of solute} \times 1000}{\text{weight of solvent in grams}} \qquad (9.25) \]Where, \( \mathrm{M_B} = \) molar mass of the solute
Therefore,
\[ \mathrm{m} = \frac{\mathrm{w_B} \times 1000}{\mathrm{M_B} \times \mathrm{w_A}} \qquad (9.27) \]and
\[ \Delta \mathrm{T_b} = \frac{\mathrm{K_b} \times \mathrm{w_B} \times 1000}{\mathrm{M_B} \times \mathrm{w_A}} \qquad (9.28) \]Molar mass can be calculated by using (9.28)
\[ \mathrm{M_B} = \frac{\mathrm{K_b} \times \mathrm{w_B} \times 1000}{\Delta \mathrm{T_b} \times \mathrm{w_A}} \qquad (9.29) \]Table 9.3 Molal boiling point elevation constant \( \mathrm{K_b} \) for some solvents
| S. No. | Solvent | \( T_b^0 (K) \) | \( K_b (K \ kg \ mol^{-1}) \) |
|---|---|---|---|
| 1. | Water | 373.15 | 0.52 |
| 2. | Ethanol | 351.5 | 1.20 |
| 3. | Benzene | 353.3 | 2.53 |
| 4. | Chloroform | 334.4 | 3.63 |
| 5. | Ether | 307.8 | 2.02 |
| 6. | Carbon tetrachloride | 350.0 | 5.03 |
| 7. | Carbon disulphide | 319.4 | 2.42 |
| 8. | Acetic acid | 391.1 | 2.93 |
| 9. | Cyclohexane | 353.74 | 2.79 |
Example Problem 4
0.75 g of an unknown substance is dissolved in \( 200 \ \mathrm{g} \) solvent. If the elevation of boiling point is \( 0.15 \ \mathrm{K} \) and molal elevation constant is \( 7.5 \ \mathrm{K \ kg \ mol^{-1}} \) then, calculate the molar mass of unknown substance.
\[ \Delta \mathrm{T_b} = \mathrm{K_b m} \]\[ = \mathrm{K_b \times \frac{w_2 \times 1000}{M_2 \times w_1}} \]\[ \mathrm{M_2 = \frac{K_b \times w_2 \times 1000}{\Delta T_b \times w_1}} \]\[ = \frac{7.5 \times 0.75 \times 1000}{0.15 \times 200} \]\[ = 187.5 \ \mathrm{g \ mol^{-1}} \]Evaluate Yourself
- 2.56 g of Sulphur is dissolved in \( 100 \ \mathrm{g} \) of carbon disulphide. The solution boils at 319.692 K. What is the molar mass of Sulphur in solution? The boiling point of \( \mathrm{CS_2} \) is 319.450 K. Given that \( \mathrm{K_b} \) for \( \mathrm{CS_2} = 2.42 \ \mathrm{K \ kg \ mol^{-1}} \).
Depression in freezing point
Freezing point of a substance is another important physical property like boiling point. Freezing point is defined as “the temperature at which the solid and the liquid states of the substance have the same vapour pressure”. At freezing point, the solid and liquid phases of the substance are in equilibrium. For example, the freezing point of water is \( 0^{\circ}C \). At this temperature the ice and water are in equilibrium. When a nonvolatile solute is added to water at its freezing point, the freezing point of the solution is lowered from \( 0^{\circ}C \). The lowering of the freezing point of the solvent when a solute is added is called depression in freezing point \( (\Delta \mathrm{T_f}) \).
From the above graph, we infer that the freezing point \( (\mathrm{T_f^{\circ}}) \) is \( 0^{\circ}C \) as the vapour pressure at this temperature is 1 atm (atmospheric pressure). The vapour pressure versus temperature curve for the solution indicates that the freezing point \( (\mathrm{T_f}) \) is lower than \( 0^{\circ}C \). The depression in freezing temperature \( (\Delta \mathrm{T_f}) \) can be expressed as,
\[ \Delta \mathrm{T_f} = \mathrm{T_f^{\circ}} - \mathrm{T_f} \]The experimental results show that the depression in freezing point is directly proportional to the molal concentration of the solute particles.
Hence,
\[ \Delta \mathrm{T_f} \propto m \]\[ \Delta \mathrm{T_f} = \mathrm{K_f} m \qquad (9.30) \]Here, \( m = \) is the molality of the solution
\( \mathrm{K_f} = \) molal freezing point depression constant or cryoscopic constant.
If \( m = 1 \), then \( \Delta \mathrm{T_f} = \mathrm{K_f} \)
The \( \mathrm{K_f} \) is equal to the depression in freezing point for 1 molal solution.
Table 9.4 Molal freezing point depression constant for some solvents
| S. No. | Solvent | Freezing point (K) | \( K_f (K \ kg \ mol^{-1}) \) |
|---|---|---|---|
| 1. | Water | 273.0 | 1.86 |
| 2. | Ethanol | 155.7 | 1.99 |
| 3. | Benzene | 278.6 | 5.12 |
| 4. | Chloroform | 209.6 | 4.79 |
| 5. | Carbon disulphide | 164.2 | 3.83 |
| 6. | Ether | 156.9 | 1.79 |
| 7. | Cyclohexane | 279.5 | 20.0 |
| 8. | Acetic acid | 290.0 | 3.90 |
Determination of molar mass of solute from depression in freezing point
If the solution is prepared by dissolving \( \mathrm{w_B} \ \mathrm{g} \) of solute in \( \mathrm{w_A} \ \mathrm{g} \) of solvent, then depression in freezing point is given by (9.31)
\[ \Delta \mathrm{T_f} = \frac{\mathrm{K_f} \times \mathrm{w_B} \times 1000}{\mathrm{M_B} \times \mathrm{w_A}} \qquad (9.31) \]Molar mass of a solute can be calculated using (9.31)
\[ \mathrm{M_B} = \frac{\mathrm{K_f} \times \mathrm{w_B} \times 1000}{\Delta \mathrm{T_f} \times \mathrm{w_A}} \qquad (9.32) \]Example Problem 5
Ethylene glycol \( \mathrm{(C_2H_6O_2)} \) can be used as an antifreeze in the radiator of a car. Calculate the temperature when ice will begin to separate from a mixture with 20 mass percent of glycol in water used in the car radiator. \( \mathrm{K_f} \) for water \( = 1.86 \ \mathrm{K \ kg \ mol^{-1}} \) and molar mass of ethylene glycol is \( 62 \ \mathrm{g \ mol^{-1}} \).
Weight of solute \( \mathrm{(W_2)} = 20 \) mass percent of solution means \( 20 \ \mathrm{g} \) of ethylene glycol
Weight of solvent (water) \( \mathrm{W_1} = 100 - 20 = 80 \ \mathrm{g} \)
\[ \Delta \mathrm{T_f} = \mathrm{K_f} m \]\[ = \frac{\mathrm{K_f} \times \mathrm{W_2} \times 1000}{\mathrm{M_2} \times \mathrm{W_1}} \]\[ = \frac{1.86 \times 20 \times 1000}{62 \times 80} \]\[ = 7.5 \ \mathrm{K} \]The temperature at which ice will begin to separate is the freezing point of water after the addition of solute i.e. \( 7.5 \ \mathrm{K} \) lower than the normal freezing point of water \( (273 - 7.5 \ \mathrm{K}) = 265.5 \ \mathrm{K} \).
Evaluate Yourself
- \( 2 \ \mathrm{g} \) of a non electrolyte solute dissolved in \( 75 \ \mathrm{g} \) of benzene lowered the freezing point of benzene by \( 0.20 \ \mathrm{K} \). The freezing point depression constant of benzene is \( 5.12 \ \mathrm{K \ kg \ mol^{-1}} \). Find the molar mass of the solute.
Osmosis and osmotic pressure
Many biological processes depend on osmosis, which is a spontaneous process by which the solvent molecules pass through a semi permeable membrane from a solution of lower concentration to a solution of higher concentration. The name osmosis is derived from the Greek word ‘osmós’ which means ’to push’. It is also important to know that the semipermeable membrane selectively allows certain molecules in the solution to pass through it but not others.
Let us consider a simple apparatus as shown in the above figure. A semipermeable membrane separates a chamber into two compartments. Water (pure solvent) is added to the first compartment and the aqueous NaCl (solution) is added to the second compartment such that the liquid levels on the both sides are equal. Since there is a difference in concentration between the liquids present in the two compartments, the water molecules move from first compartment to second compartment through the semipermeable membrane. The membrane allows only water molecules to pass through it in either direction but not NaCl. The net flow of water is into the sodium chloride solution and hence increases its volume. This decreases its concentration and also creates a pressure difference between the compartments. This pressure difference pushes some of the water molecules back to the solvent side through the semipermeable membrane until an equilibrium is established. At the equilibrium, the rate of movement of solvent molecules in both directions are equal. The pressure difference at the equilibrium is called osmotic pressure \( (\pi) \). Thus, osmotic pressure can be defined as “the pressure that must be applied to the solution to stop the influx of the solvent (to stop osmosis) through the semipermeable membrane”.
van’t Hoff found out that for dilute solutions, the osmotic pressure is directly proportional to the molar concentration of the solute and the temperature of the solution. He proposed the following equation to calculate osmotic pressure which is now called as van’t Hoff equation.
\[ \pi = \mathrm{CRT} \qquad (9.31) \]Here, \( \mathrm{C} = \) Concentration of the solution in molarity \( \mathrm{T} = \) Temperature \( \mathrm{R} = \) Gas constant
Determination of molar mass from osmotic pressure
According to van’t Hoff equation
\[ \pi = \mathrm{CRT} \]\[ \mathrm{C} = \frac{\mathrm{n}}{\mathrm{V}} \]Here, \( \mathrm{n} = \) number of moles of solute dissolved in \( \mathrm{V} \) litre of the solution.
Therefore,
\[ \pi = \frac{\mathrm{n}}{\mathrm{V}} \mathrm{RT} \quad \text{or} \quad \pi \mathrm{V} = \mathrm{nRT} \qquad (9.33) \]If the solution is prepared by dissolving \( \mathrm{w_B} \ \mathrm{g} \) of nonvolatile solute in \( \mathrm{w_A} \ \mathrm{g} \) of solvent, then the number of moles of solute (n) is,
\[ \mathrm{n} = \mathrm{w_B} / \mathrm{M_B} \]Here, \( \mathrm{M_B} = \) molar mass of the solute
Substituting the ’n’ in (9.33), we get,
\[ \pi = \frac{\mathrm{w_B}}{\mathrm{V}} \frac{\mathrm{RT}}{\mathrm{M_B}} \]\[ \mathrm{M_B} = \frac{\mathrm{w_B}}{\mathrm{V}} \frac{\mathrm{RT}}{\pi} \qquad (9.34) \]From the equation 9.33, molar mass of the solute can be calculated.
Significances of osmotic pressure over other colligative properties
- Unlike elevation of boiling point (for 1 molal solution the elevation in boiling point is \( 0.512^{\circ}C \) for water) and the depression in freezing point (for 1 molal solution the depression in freezing point is \( 1.86^{\circ}C \) for water), the magnitude of osmotic pressure is large.
- The osmotic pressure can be measured at room temperature which enables to determine the molecular mass of biomolecules which are unstable at higher temperatures.
- Even for a very dilute solution, the osmotic pressure is large.
Isotonic solutions
Two solutions having same osmotic pressure at a given temperature are called isotonic solutions. When such solutions are separated by a semipermeable membrane, solvent flow between one to the other on either direction is same, i.e. the net solvent flow between the two isotonic solutions is zero.
The osmotic pressure of the blood cells is approximately equal to 7 atm at \( 37^{\circ}C \). The intravenous injections should have same osmotic pressure as that of the blood (isotonic with blood). If the Intravenous solutions are too dilute that is hypotonic, the solvent from outside of the cells will flow into the cell to normalise the osmotic pressure and this process which is called hemolysis, causes the cells to burst. On the other hand, if the solution is too concentrated, that is hypertonic, the solvent molecules will flow out of the cells, which causes the cells to shrink and die. For this reason, the Intravenous fluids are prepared such they are isotonic to blood \( (0.9\%) \) mass/volume sodium chloride solution).
9.10 Reverse osmosis (RO)
Let us consider the experimental setup discussed in the osmosis. The pure water moves through the semipermeable membrane to the NaCl solution due to osmosis. This process can be reversed by applying pressure greater than the osmotic pressure to the solution side. Now the pure water moves from the solution side to the solvent side and this process is called reverse osmosis. It can be defined as a process in which a solvent passes through a semipermeable membrane in the opposite direction of osmosis, when subjected to a hydrostatic pressure greater than the osmotic pressure.
Application of Reverse osmosis in water purification
Reverse osmosis is used in the desalination of sea water and also in the purification of drinking water. A simple set up used in both the process is shown in the figure 9.15. When a pressure higher than the osmotic pressure is applied on the solution side (sea water) the water molecules moves from solution side to the solvent side through semipermeable membrane (Opposite to the Osmotic flow). Pure water can be collected. There are different types of semipermeable membranes used in this process. The membrane used for reverse osmosis has to withstand high pressures. Generally, cellulose acetate or polyamide membranes are commonly used in commercial systems. The selection of membrane used for reverse osmosis will be decided based on the nature of the input water.
Example Problem 6
At \( 400 \ \mathrm{K} \), \( 1.5 \ \mathrm{g} \) of an unknown substance is dissolved in a solvent and the solution is made to \( 1.5 \ \mathrm{L} \). Its osmotic pressure is found to be 0.3 bar. Calculate the molar mass of the unknown substance.
\[ \mathrm{Molar \ mass} = \frac{\text{mass of unknown solute} \times \mathrm{RT}}{\text{osmotic pressure} \times \text{volume of solution}} \]\[ = \frac{1.5 \times 8.314 \times 10^{-2} \times 400}{0.3 \times 1.5} \]\[ = 110.85 \ \mathrm{g \ mol^{-1}} \]Evaluate Yourself
- What is the mass of glucose \( \mathrm{(C_6H_{12}O_6)} \) in one litre solution which is isotonic with \( 6 \ \mathrm{g \ L^{-1}} \) of urea \( \mathrm{(NH_2CONH_2)} \)?
9.11 Abnormal molar mass
The molar masses of the nonvolatile solutes can be calculated accurately using the experimentally determined colligative properties. In this method, we assume that the solution is very dilute and there is no dissociation or association of solute particles in the solution.
In a concentrated solution, the interaction between the solute and solvent becomes significant and reflected in the measured colligative properties. Similarly, the dissociation or association of solute molecules would alter the total number of particles present in the solution and hence affect the results of measured colligative properties. In such solutions, the value of the molar mass of the solute determined using colligative properties would be different from the actual molar mass, and it is called abnormal molar mass.
Association or dissociation of solute molecules
Normally, the molar mass determination using measured colligative properties assumes that the solute does not dissociate or associate. In certain solvents, solute molecules associate to form a dimer or trimer etc. This reduces the total number of particles (molecules) formed in solution and as a result the calculated molar mass will be higher than the actual molar mass. Let us consider a solution of acetic acid in benzene. It is already established that acetic acid forms intermolecular hydrogen bonds as shown in the figure 9.9 and exists as a dimer in benzene.
\[ 2\mathrm{CH_3COOH} \rightarrow (\mathrm{CH_3COOH})_2 \]The molar mass of acetic acid calculated using colligative properties is found to be around \( 120 \ \mathrm{g \ mol^{-1}} \) which is two times the actual molar mass \( (60 \ \mathrm{g \ mol^{-1}}) \).
The electrolytes such as KCl or NaCl dissociates completely into its constituent ions in their aqueous solution. This causes an increase in the total number of particles (ions) present in the solution. The calculated molar mass using colligative property measurement for this type of solutions will be lower than the actual molar mass. For example, sodium chloride dissociates into \( \mathrm{Na^{+}} \) ions and \( \mathrm{Cl^{-}} \) ions in aqueous solution, as shown below.
\[ \mathrm{NaCl(s)} \rightarrow \mathrm{Na^{+}(aq)} + \mathrm{Cl^{-}(aq)} \]When we dissolve 1 mole of NaCl \( (58.4 \ \mathrm{g}) \) in water, it dissociates and gives 1 mole of \( \mathrm{Na^{+}} \) and 1 mole of \( \mathrm{Cl^{-}} \). Hence, the solution will have 2 moles of particles. Thus, the colligative properties would be double the expected value.
van’t Hoff factor
We have learnt that the dissociation or association of solute molecules in a solution will result in the increase or decrease in the calculated molar mass using the colligative property. This variation is proportional to the extent of association or dissociation. To quantify the extent of association or dissociation of solutes in solution, van’t Hoff introduced a term ‘i’ which is now called van’t Hoff factor. It is defined as the ratio of the actual molar mass to the abnormal (calculated) molar mass of the solute. Here, the abnormal molar mass is the molar mass calculated using the experimentally determined colligative property.
\[ i = \frac{\text{Normal (actual) molar mass}}{\text{Observed (abnormal) molar mass}} = \frac{\text{Observed colligative property}}{\text{Calculated colligative property}} \]The estimated van’t Hoff factor for acetic acid solution in Benzene is 0.5 and that of sodium chloride solution in water is 2. The degree of dissociation or association can be related to Van’t Hoff factor (i) using the following relationships
\[ \alpha_{\text{dissociation}} = \frac{i - 1}{n - 1} \](Where n is number ions/species formed by the dissociation of a single molecule)
\[ \alpha_{\text{association}} = \frac{(1 - i)n}{n - 1} \](Here, n is the number of solute molecules involved in association.)
The equations relating the four colligative properties with the concentration of the solutes can be rewritten as follows by incorporating the van’t Hoff factor
Relative lowering of vapour pressure,
\[ \frac{P_{\text{solvent}}^{\circ} - P_{\text{solution}}}{P_{\text{solvent}}^{\circ}} = i \frac{n_{\text{solute}}}{n_{\text{solvent}}} \]Elevation of boiling point
\[ \Delta T_b = i K_b m \]Depression in the freezing point
\[ \Delta T_f = i K_f m \]Osmotic pressure
\[ \pi = i \frac{w_{\text{solute}}}{V} \frac{RT}{M_{\text{solute}}} \]For a solute that does not dissociate or associate the van’t Hoff factor is equal to 1 (i = 1) and the molar mass will be close to the actual molar mass.
For the solutes that associate to form higher oligomers in solution the van’t Hoff factor will be less than one (i < 1) and the observed molar mass will be greater than the actual molar mass.
For solutes that dissociates into their constituent ions the van’t Hoff factor will be more than one (i > 1) and the observed molar mass will be less than the normal molar mass.
Example Problem 7
The depression in freezing point is 0.24 K obtained by dissolving 1 g NaCl in 200 g water. Calculate van’t-Hoff factor. The molal depression constant is 1.86 K kg mol\(^{-1}\)
Molar mass of solute
\[ = \frac{1000 \times K_f \times \text{mass of NaCl}}{\Delta T_f \times \text{mass of solvent}} \]\[ = \frac{1000 \times 1.86 \times 1}{0.24 \times 200} \]\[ = 38.75 \ \mathrm{g \ mol^{-1}} \]Theoretical molar mass of NaCl is \( 58.5 \ \mathrm{g \ mol^{-1}} \)
\[ i = \frac{\text{Theoretical molar mass}}{\text{Experimental molar mass}} = \frac{58.5}{38.75} = 1.50 \]Evaluate Yourself
- 0.2 m aqueous solution of KCl freezes at -0.68°C. Calculate van’t Hoff factor. \( K_f \) for water is 1.86 K kg mol\(^{-1}\).
Summary
A solution is a homogeneous mixture of two or more chemically nonreacting substances mixed uniformly. The proportion of component which is more in the solution is called solvent and the lesser component is called solute.
The different concentration units used to prepare the solutions are formality, molality, normality, molality, mole fraction, \( \% w/w \) solution, \( \% w/v \) solution, \( \% v/v \) solution. If the solute quantity is very minimum then ppm unit is used to express its concentration.
The standard solutions are prepared and diluted to desired concentration (working standards). This helps in overcoming the error due to weighing and maintain efficiency and consistency in the preparation of solution.
Solubility is defined as the amount of solute in a saturated solution per \( 100 \ \mathrm{g} \) of a solvent. Solubility of a solute in a solvent depends on the nature of the solute and solvent, temperature.
The solubility of a gas in a liquid depends upon, the nature of the gas and the nature of the liquid, the temperature of the system, and the pressure of the gas.
The effect of pressure on the solubility of a gas in a liquid is governed by Henry’s Law. It states that the solubility of a gas in a liquid at a given temperature is directly proportional to the partial pressure of the gas.
The vapour pressure of a liquid is the pressure exerted by its vapour when it is in dynamic equilibrium with its liquid, in a closed container. According to Raoults Law, the vapour pressure of a solution containing a non-volatile solute is directly proportional to the mole fraction of the solvent \( (\mathrm{X_A}) \). The proportionality constant being the vapour pressure of the pure solvent.
The solution shows positive deviation from Raoult’s Law if its vapour pressure is higher than that predicted by Raoult’s Law for example ethyl alcohol and cyclohexane.
The solution shows negative deviation if its vapour pressure is lower than that predicted by Raoult’s Law for example acetone and chloroform.
Colligative properties of solutions are those properties which depend only upon the number of solute particles in the solution and not on their nature. Such properties are
(a) Relative lowering in vapour pressure: On addition of a non volatile solute it is observed that the vapour pressure of the solution is lesser than the solvent. According to Raoult’s law relative lowering of vapour pressure is equal to the mole fraction of the solute.
(b) Elevation of boiling point \( \Delta \mathrm{T_b} \): The solution boils at a higher temperature than the pure solvent. This is due to the decreased vapour pressure of solution and the temperature it reaches the atmospheric pressure on heating to boil is much higher than the solvent.
(c) Depression of freezing point: The freezing point of the solution is much lower than the solvent as the temperature at which the solid and the liquid have the same vapour pressure is much lower than the solvent.
(d) Osmotic pressure: The spontaneous flow of solvent molecules from a dilute solution into a concentrated solution when the two are separated by a perfect semipermeable membrane is called osmosis.
Osmotic pressure \( (\pi) \) is the pressure which must be applied to the solution side (more concentrated solution) to just prevent the passage of pure solvent into it through a semipermeable membrane.
Abnormal colligative properties
If solutes undergo any association or dissociation in a solution, they exhibit abnormal colligative properties. Van’t Hoff factor explains quantitatively the extent of association or dissociation of solutes in solvent.
Evaluation
I. Choose the best answer.
The molality of a solution containing \( 1.8 \ \mathrm{g} \) of glucose dissolved in \( 250 \ \mathrm{g} \) of water is a) \( 0.2 \ \mathrm{M} \) b) \( 0.01 \ \mathrm{M} \) c) \( 0.02 \ \mathrm{M} \) d) \( 0.04 \ \mathrm{M} \)
Which of the following concentration terms is / are independent of temperature a) molality b) molarity c) mole fraction d) (a) and (c)
Stomach acid, a dilute solution of HCl can be neutralised by reaction with Aluminium hydroxide
\[ \mathrm{Al(OH)_3 + 3HCl(aq) \rightarrow AlCl_3 + 3H_2O} \]How many millilitres of \( 0.1 \ \mathrm{M} \ \mathrm{Al(OH)_3} \) solution are needed to neutralise \( 21 \ \mathrm{mL} \) of \( 0.1 \ \mathrm{M} \ \mathrm{HCl} \)? a) \( 14 \ \mathrm{mL} \) b) \( 7 \ \mathrm{mL} \) c) \( 21 \ \mathrm{mL} \) d) none of these
The partial pressure of nitrogen in air is 0.76 atm and its Henry’s law constant is \( 7.6 \times 10^{4} \) atm at \( 300 \ \mathrm{K} \). What is the mole fraction of nitrogen gas in the solution obtained when air is bubbled through water at \( 300 \ \mathrm{K} \)? a) \( 1 \times 10^{-4} \) b) \( 1 \times 10^{-6} \) c) \( 2 \times 10^{-5} \) d) \( 1 \times 10^{-5} \)
The Henry’s law constant for the solubility of Nitrogen gas in water at \( 350 \ \mathrm{K} \) is \( 8 \times 10^{4} \) atm. The mole fraction of nitrogen in air is 0.5. The number of moles of Nitrogen from air dissolved in 10 moles of water at \( 350 \ \mathrm{K} \) and 4 atm pressure is a) \( 4 \times 10^{-4} \) b) \( 4 \times 10^{4} \) c) \( 2 \times 10^{-2} \) d) \( 2.5 \times 10^{-4} \)
Which one of the following is incorrect for ideal solution? a) \( \Delta \mathrm{H_{mix}} = 0 \) b) \( \Delta \mathrm{U_{mix}} = 0 \) c) \( \Delta \mathrm{P} = \mathrm{P_{observed}} - \mathrm{P_{calculated \ by \ Raoults \ law}} = 0 \) d) \( \Delta \mathrm{G_{mix}} = 0 \)
Which one of the following gases has the lowest value of Henry’s law constant? a) \( \mathrm{N_2} \) b) \( \mathrm{He} \) c) \( \mathrm{CO_2} \) d) \( \mathrm{H_2} \)
\( \mathrm{P_1} \) and \( \mathrm{P_2} \) are the vapour pressures of pure liquid components, 1 and 2 respectively of an ideal binary solution if \( \mathbf{x_1} \) represents the mole fraction of component 1, the total pressure of the solution formed by 1 and 2 will be a) \( \mathrm{P_1 + x_1(P_2 - P_1)} \) b) \( \mathrm{P_2 - x_1(P_2 + P_1)} \) c) \( \mathrm{P_1 - x_2(P_1 - P_2)} \) d) \( \mathrm{P_1 + x_2(P_1 - P_2)} \)
Osmotic pressure \( (\pi) \) of a solution is given by the relation a) \( \pi = \mathrm{nRT} \) b) \( \pi \mathrm{V} = \mathrm{nRT} \) c) \( \pi \mathrm{RT} = \mathrm{n} \) d) none of these
Which one of the following binary liquid mixtures exhibits positive deviation from Raoults law? a) Acetone + chloroform b) Water + nitric acid c) HCl + water d) ethanol + water
The Henry’s law constants for two gases A and B are \( \mathbf{x} \) and \( \mathbf{y} \) respectively. The ratio of mole fractions of A to B is 0.2. The ratio of mole fraction of B and A dissolved in water will be a) \( \frac{2x}{y} \) b) \( \frac{y}{0.2x} \) c) \( \frac{0.2x}{y} \) d) \( \frac{5x}{y} \)
At \( 100^{\circ}C \) the vapour pressure of a solution containing \( 6.5 \ \mathrm{g} \) a solute in \( 100 \ \mathrm{g} \) water is \( 732 \ \mathrm{mm} \). If \( \mathrm{K_b} = 0.52 \), the boiling point of this solution will be a) \( 102^{\circ}C \) b) \( 100^{\circ}C \) c) \( 101^{\circ}C \) d) \( 100.52^{\circ}C \)
According to Raoults law, the relative lowering of vapour pressure for a solution is equal to a) mole fraction of solvent b) mole fraction of solute c) number of moles of solute d) number of moles of solvent
At same temperature, which pair of the following solutions are isotonic? a) \( 0.2 \ \mathrm{M} \ \mathrm{BaCl_2} \) and \( 0.2 \ \mathrm{M} \) urea b) \( 0.1 \ \mathrm{M} \) glucose and \( 0.2 \ \mathrm{M} \) urea c) \( 0.1 \ \mathrm{M} \) NaCl and \( 0.1 \ \mathrm{M} \ \mathrm{K_2SO_4} \) d) \( 0.1 \ \mathrm{M} \ \mathrm{Ba(NO_3)_2} \) and \( 0.1 \ \mathrm{M} \ \mathrm{Na_2SO_4} \)
The empirical formula of a non-electrolyte(X) is \( \mathrm{CH_2O} \). A solution containing six gram of X exerts the same osmotic pressure as that of \( 0.025 \ \mathrm{M} \) glucose solution at the same temperature. The molecular formula of X is a) \( \mathrm{C_2H_4O_2} \) b) \( \mathrm{C_8H_{16}O_8} \) c) \( \mathrm{C_4H_8O_4} \) d) \( \mathrm{CH_2O} \)
The \( \mathrm{K_H} \) for the solution of oxygen dissolved in water is \( 4 \times 10^{4} \) atm at a given temperature. If the partial pressure of oxygen in air is 0.4 atm, the mole fraction of oxygen in solution is a) \( 4.6 \times 10^{3} \) b) \( 1.6 \times 10^{4} \) c) \( 1 \times 10^{-5} \) d) \( 1 \times 10^{5} \)
Normality of \( 1.25 \ \mathrm{M} \) sulphuric acid is a) \( 1.25 \ \mathrm{N} \) b) \( 3.75 \ \mathrm{N} \) c) \( 2.5 \ \mathrm{N} \) d) \( 2.25 \ \mathrm{N} \)
Two liquids X and Y on mixing gives a warm solution. The solution is a) ideal b) non-ideal and shows positive deviation from Raoults law c) ideal and shows negative deviation from Raoults Law d) non-ideal and shows negative deviation from Raoults Law
The relative lowering of vapour pressure of a sugar solution in water is \( 3.5 \times 10^{-3} \). The mole fraction of water in that solution is a) \( 0.0035 \) b) \( 0.35 \) c) \( 0.0035 / 18 \) d) \( 0.9965 \)
The mass of a non-volatile solute (molar mass \( 80 \ \mathrm{g \ mol^{-1}} \)) which should be dissolved in \( 92 \ \mathrm{g} \) of toluene to reduce its vapour pressure to \( 90\% \) a) \( 10 \ \mathrm{g} \) b) \( 20 \ \mathrm{g} \) c) \( 9.2 \ \mathrm{g} \) d) \( 8.89 \ \mathrm{g} \)
For a solution, the plot of osmotic pressure \( (\pi) \) verses the concentration (c in mol \( \mathrm{L^{-1}} \)) gives a straight line with slope \( 310 \mathrm{R} \) where ‘R’ is the gas constant. The temperature at which osmotic pressure measured is a) \( 310 \times 0.082 \ \mathrm{K} \) b) \( 310^{\circ}C \) c) \( 37^{\circ}C \) d) \( \frac{310}{0.082} \ \mathrm{K} \)
\( 200 \ \mathrm{ml} \) of an aqueous solution of a protein contains \( 1.26 \ \mathrm{g} \) of protein. At \( 300 \ \mathrm{K} \), the osmotic pressure of this solution is found to be \( 2.52 \times 10^{-3} \) bar. The molar mass of protein will be \( (\mathrm{R} = 0.083 \ \mathrm{L \ bar \ mol^{-1} \ K^{-1}}) \) a) \( 62.22 \ \mathrm{Kg \ mol^{-1}} \) b) \( 12444 \ \mathrm{g \ mol^{-1}} \) c) \( 300 \ \mathrm{g \ mol^{-1}} \) d) none of these
The Van’t Hoff factor (i) for a dilute aqueous solution of the strong electrolyte barium hydroxide is (NEET) a) 0 b) 1 c) 2 d) 3
What is the molality of a \( 10\% \ \mathrm{W/W} \) aqueous sodium hydroxide solution? a) 2.778 b) 2.5 c) 10 d) 0.4
The correct equation for the degree of an associating solute, ’n’ molecules of which undergoes association in solution, is a) \( \alpha = \frac{n(i - 1)}{n - 1} \) b) \( \alpha^2 = \frac{n(i - 1)}{(n - 1)} \) c) \( \alpha = \frac{n(i - 1)}{1 - n} \) d) \( \alpha = \frac{n(1 - i)}{n(1 - i)} \)
Which of the following aqueous solutions has the highest boiling point? a) \( 0.1 \ \mathrm{M} \ \mathrm{KNO_3} \) b) \( 0.1 \ \mathrm{M} \ \mathrm{Na_3PO_4} \) c) \( 0.1 \ \mathrm{M} \ \mathrm{BaCl_2} \) d) \( 0.1 \ \mathrm{M} \ \mathrm{K_2SO_4} \)
The freezing point depression constant for water is \( 1.86^{\circ} \mathrm{K \ kg \ mol^{-1}} \). If \( 5 \ \mathrm{g} \ \mathrm{Na_2SO_4} \) is dissolved in \( 45 \ \mathrm{g} \) water, the depression in freezing point is \( 3.64^{\circ}C \). The Van’t Hoff factor for \( \mathrm{Na_2SO_4} \) is a) 2.50 b) 2.63 c) 3.64 d) 5.50
Equimolal aqueous solutions of NaCl and KCl are prepared. If the freezing point of NaCl is \( -2^{\circ}C \), the freezing point of KCl solution is expected to be a) \( -2^{\circ}C \) b) \( -4^{\circ}C \) c) \( -1^{\circ}C \) d) \( 0^{\circ}C \)
Phenol dimerises in benzene having van’t Hoff factor 0.54. What is the degree of association? a) 0.46 b) 92 c) 46 d) 0.92
Assertion: An ideal solution obeys Raoults Law Reason: In an ideal solution, solvent-solvent as well as solute-solute interactions are similar to solute-solvent interactions. a) both assertion and reason are true and reason is the correct explanation of assertion b) both assertion and reason are true but reason is not the correct explanation of assertion c) assertion is true but reason is false d) both assertion and reason are false
II. Write brief answer to the following questions
Define (i) molality (ii) Normality
What is a vapour pressure of liquid? What is relative lowering of vapour pressure?
State and explain Henry’s law
State Raoult law and obtain expression for lowering of vapour pressure when nonvolatile solute is dissolved in solvent.
What is molal depression constant? Does it depend on nature of the solute?
What is osmosis?
Define the term ‘isotonic solution’.
You are provided with a solid ‘A’ and three solutions of A dissolved in water - one saturated, one unsaturated, and one super saturated. How would you determine which solution is which?
Explain the effect of pressure on the solubility.
A sample of 12 M Concentrated hydrochloric acid has a density 1.2 g L\(^{-1}\). Calculate the molality.
A 0.25 M glucose solution at 370.28 K has approximately the same osmotic pressure as blood does. What is the osmotic pressure of blood?
Calculate the molality of a solution containing \( 7.5 \ \mathrm{g} \) of glycine \( (\mathrm{NH_2 - CH_2 - COOH}) \) dissolved in \( 500 \ \mathrm{g} \) of water.
Which solution has the lower freezing point? \( 10 \ \mathrm{g} \) of methanol \( (\mathrm{CH_3OH}) \) in \( 100 \ \mathrm{g} \) of water (or) \( 20 \ \mathrm{g} \) of ethanol \( (\mathrm{C_2H_5OH}) \) in \( 200 \ \mathrm{g} \) of water.
How many moles of solute particles are present in one litre of \( 10^{-4} \ \mathrm{M} \) potassium sulphate?
Henry’s law constant for solubility of methane in benzene is \( 4.2 \times 10^{-5} \ \mathrm{mm} \ \mathrm{Hg} \) at a particular constant temperature. At this temperature, calculate the solubility of methane at i) \( 750 \ \mathrm{mm} \ \mathrm{Hg} \) ii) \( 840 \ \mathrm{mm} \ \mathrm{Hg} \)
The observed depression in freezing point of water for a particular solution is \( 0.093^{\circ}C \). Calculate the concentration of the solution in molality. Given that molal depression constant for water is \( 1.86 \ \mathrm{K \ kg \ mol^{-1}} \).
The vapour pressure of pure benzene \( (\mathrm{C_6H_6}) \) at a given temperature is \( 640 \ \mathrm{mm} \ \mathrm{Hg} \). \( 2.2 \ \mathrm{g} \) of non-volatile solute is added to \( 40 \ \mathrm{g} \) of benzene. The vapour pressure of the solution is \( 600 \ \mathrm{mm} \ \mathrm{Hg} \). Calculate the molar mass of the solute.
ICT Corner
Osmosis
By using this tool, you will be able to visualise the process of osmosis which gives a clear understanding of this process.
Please go to the URL https://pbslm-contrib.s3.amazonaws.com/WGBH/arct15/SimBucket/Simulations/osmosis/content/index.html (or) Scan the QR code on the right side.
Steps
- Open the Browser and type the URL given (or) Scan the QR Code.
- Now you will see the webpage as shown below.
- The two compartments were separated by a semipermeable membrane.
- On the left side (Box 2) contains pure solvent (water) and right side contains solution (solute + water).
- The number of solvent molecules (water) on each side is shown in the area designated by box 3 and 5.
- Now you can see the water molecules moving from solvent side to solution side through the membrane. It reflects in the change in number of water molecules on either side.
- You can restart the simulation by clicking the reset button in box 1.