Problem 126
Question
An aqueous solution of a solute which neither associates nor dissociates has a freezing point depression of \(\mathrm{X}^{\circ} \mathrm{C}\). An equimolar solution of a second has a freezing point depression of \(4 \mathrm{X}^{\circ} \mathrm{C}\). The second solution could be a salt of formula (assuming \(100 \%\) dissociation ) (a) \(\mathrm{AB}_{2}\) (b) \(\mathrm{A}_{2} \mathrm{~B}_{2}\) (c) \(\mathrm{A}_{3} \mathrm{~B}\) (d) \(\mathrm{AB}_{3}\)
Step-by-Step Solution
Verified Answer
The second solution could be \( \mathrm{A}_2\mathrm{B}_2 \), \( \mathrm{A}_3\mathrm{B} \) or \( \mathrm{AB}_3 \).
1Step 1: Understanding Freezing Point Depression
The freezing point depression is a colligative property that depends on the number of solute particles in a solution. It can be calculated using the formula \( \Delta T_f = i \cdot K_f \cdot m \), where \( \Delta T_f \) is the freezing point depression, \( i \) is the van't Hoff factor, \( K_f \) is the cryoscopic constant, and \( m \) is the molality of the solution. For the first solute, since it neither associates nor dissociates, \( i = 1 \).
2Step 2: Comparing Freezing Point Depression
The equimolar solution of the second solute has a freezing point depression \( 4X^{\circ}C \) compared to \( X^{\circ}C \) for the first solute. This implies the van't Hoff factor for the second solute, \( i_2 \), is 4 times that of the first solute. Therefore, \( i_2 = 4 \).
3Step 3: Analyzing Possible Solute Formulas
Since the second solute dissociates completely into ions, the formula must result in 4 moles of ions per mole of solute. Checking each provided option:- \( \mathrm{AB}_2 \) dissociates into \( 1A^+ + 2B^- \), total ions = 3.- \( \mathrm{A}_2\mathrm{B}_2 \) dissociates into \( 2A^+ + 2B^- \), total ions = 4.- \( \mathrm{A}_3\mathrm{B} \) dissociates into \( 3A^+ + 1B^- \), total ions = 4.- \( \mathrm{AB}_3 \) dissociates into \( 1A^+ + 3B^- \), total ions = 4.
4Step 4: Determining the Correct Formula
Options \( \mathrm{A}_2\mathrm{B}_2 \), \( \mathrm{A}_3\mathrm{B} \), and \( \mathrm{AB}_3 \) each give 4 ions upon dissociation, matching the required van't Hoff factor of 4. Thus, these formulas are possible, but without any canonical order constraint, list them as equivalent possible options.
Key Concepts
Freezing Point DepressionVan't Hoff FactorComplete DissociationEquimolar Solutions
Freezing Point Depression
Freezing point depression refers to the lowering of a liquid's freezing point by adding solute particles. When we dissolve a solute in a solvent, the presence of solute particles disturbs the formation of a structured solid, thereby lowering the temperature required for the liquid to solidify.
This phenomenon is explained by the colligative property, meaning it depends on the number of solute particles, rather than their nature.
Its magnitude can be calculated using the equation: \[ \Delta T_f = i \cdot K_f \cdot m \]where:
This phenomenon is explained by the colligative property, meaning it depends on the number of solute particles, rather than their nature.
Its magnitude can be calculated using the equation: \[ \Delta T_f = i \cdot K_f \cdot m \]where:
- \( \Delta T_f \) is the freezing point depression (the change in freezing point).
- \( i \) is the van't Hoff factor, indicating how many particles a solute produces in solution.
- \( K_f \) is the cryoscopic constant, specific to each solvent.
- \( m \) is the molality of the solution, measuring moles of solute per kilogram of solvent.
Van't Hoff Factor
The van't Hoff factor, denoted as \( i \), is crucial in calculating colligative properties like freezing point depression. It signifies the number of particles that a solute produces in solution.
For a solute that doesn't dissociate or associate in solution, \( i \) is typically 1. This means each solute molecule stays intact and forms one particle in the solution.
For a solute that doesn't dissociate or associate in solution, \( i \) is typically 1. This means each solute molecule stays intact and forms one particle in the solution.
- Non-electrolytes, like sugar, have an \( i \) value of 1.
- Electrolytes, which dissociate into ions, have \( i > 1 \).
Complete Dissociation
Complete dissociation refers to a solute entirely separating into individual ions when dissolved in a solution. This is common in strong electrolytes, such as ionic salts.
For example, a formula of \( \mathrm{A}_2\mathrm{B}_2 \) dissolving will yield 4 ions. This property is why solutions with complete dissociation have larger van't Hoff factors, as more particles mean a greater impact on properties like freezing point depression.
- For instance, NaCl dissociates fully into Na\(^+\) and Cl\(^-\) ions.
- Strong acids and bases also tend to completely dissociate in water.
For example, a formula of \( \mathrm{A}_2\mathrm{B}_2 \) dissolving will yield 4 ions. This property is why solutions with complete dissociation have larger van't Hoff factors, as more particles mean a greater impact on properties like freezing point depression.
Equimolar Solutions
Equimolar solutions have equal molar concentrations of solutes, meaning they contain the same amount of moles of solute per volume.
These solutions enable direct comparison of colligative properties because differences in behavior are due purely to the nature of the solutes, rather than their amounts.
When encountering a scenario like the one described, where two equimolar solutions have drastically different freezing point depressions, it highlights the role of particle number in colligative effects.
These solutions enable direct comparison of colligative properties because differences in behavior are due purely to the nature of the solutes, rather than their amounts.
When encountering a scenario like the one described, where two equimolar solutions have drastically different freezing point depressions, it highlights the role of particle number in colligative effects.
- A non-dissociating solute leads to fewer particles, thus a smaller impact.
- Dissociating solutes increase particle count, amplifying properties like freezing point depression.
Other exercises in this chapter
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