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12.10:

Freezing Point Depression and Boiling Point Elevation

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Chemistry
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JoVE Core Chemistry
Freezing Point Depression and Boiling Point Elevation

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The temperature at which the vapor pressure of a liquid equals the atmospheric pressure is known as its boiling point.  Since adding a non-volatile solute lowers the vapor pressure of a solvent, a solution requires a higher temperature to increase its vapor pressure to a point that equals the atmospheric pressure. Thus, the boiling point of a solution is greater than that of a pure solvent. These changes in vaporization can be examined over a range of temperatures and pressure using a phase diagram. A solution has a lower vapor pressure than the pure solvent at all temperatures. So, the vaporization curve of the solution would lie below that of the solvent.  At 1 atm, the curve corresponds to a temperature higher than the boiling point of the pure solvent.  The increase in the boiling point of the solution compared to that of the pure solvent is known as boiling point elevation. The boiling point of a solution is a colligative property. The temperature increase, or ΔTb, is directly proportional to the concentration of solute and can be calculated by multiplying the molality of the solute and the molal boiling point elevation constant. The boiling point elevation constant has the units °C per molality, and is different for each solvent. For water, the constant is 0.512 °C per molal.  So, a 2.00 molal aqueous solution will elevate the boiling point of water by 1.02 °C to 101.02 °C. The addition of a non-volatile solute also lowers the freezing point of the solution compared to that of a pure solvent. At the triple point, the vapor pressures of the solid, liquid, and gaseous states are equal.  Because a non-volatile solute lowers the vapor pressure of the solution, the entire freezing curve, which extends upward from the triple point, shifts such that the solution freezes at a lower temperature. This decrease in the freezing temperature of a solution compared to that of a pure solvent is known as freezing point depression. Like the boiling point, the freezing point of a solution is also a colligative property.  The temperature decrease or ΔTf is directly proportional to the concentration of solute and can be calculated by multiplying the molality of the solute and the molal freezing point depression constant. The freezing point depression constant also depends on the solvent and has the units °C/m. For water, the freezing point depression constant is 1.86 °C per molal. Thus, a 0.5 molal glycol solution will lower the freezing point of water by 0.93 °C to −0.93 °C.

12.10:

Freezing Point Depression and Boiling Point Elevation

Boiling Point Elevation

The boiling point of a liquid is the temperature at which its vapor pressure is equal to ambient atmospheric pressure. Since the vapor pressure of a solution is lowered due to the presence of nonvolatile solutes, it stands to reason that the solution’s boiling point will subsequently be increased. Vapor pressure increases with temperature, and so a solution will require a higher temperature than will pure solvent to achieve any given vapor pressure, including one equivalent to that of the surrounding atmosphere. The increase in boiling point observed when a non-volatile solute is dissolved in a solvent, ΔTb, is called boiling point elevation and is directly proportional to the molal concentration of solute species:

Eq1

where Kb is the boiling point elevation constant, or the ebullioscopic constant and m is the molal concentration (molality) of all solute species. Boiling point elevation constants are characteristic properties that depend on the identity of the solvent.

Freezing Point Depression

Solutions freeze at lower temperatures than pure liquids. This phenomenon is exploited in “de-icing” schemes that use salt, calcium chloride, or urea to melt ice on roads and sidewalks, and in the use of ethylene glycol as an “antifreeze” in automobile radiators. Seawater freezes at a lower temperature than freshwater, and so the Arctic and Antarctic oceans remain unfrozen even at temperatures below 0 °C (as do the body fluids of fish and other cold-blooded sea animals that live in these oceans).

The decrease in freezing point of a dilute solution compared to that of the pure solvent, ΔTf, is called the freezing point depression and is directly proportional to the molal concentration of the solute

Eq2

where m is the molal concentration of the solute and Kf is called the freezing point depression constant (or cryoscopic constant). Just as for boiling point elevation constants, these are characteristic properties whose values depend on the chemical identity of the solvent.

Determination of Molar Masses

Osmotic pressure and changes in freezing point, boiling point, and vapor pressure are directly proportional to the number of solute species present in a given amount of solution. Consequently, measuring one of these properties for a solution prepared using a known mass of solute permits determination of the solute’s molar mass.

For example, a solution of 4.00 g of a nonelectrolyte dissolved in 55.0 g of benzene is found to freeze at 2.32 °C. Assuming ideal solution behavior, what is the molar mass of this compound?

To solve this problem, first, the change in freezing point from the observed freezing point and the freezing point of pure benzene is calculated:

Eq3

Then, the molal concentration is determined from Kf, the freezing point depression constant for benzene, and ΔTf:

Eq4

Next, the number of moles of the compound in the solution is found from the molal concentration and the mass of solvent that was used to make the solution.

Eq5

And, finally, the molar mass from the mass of the solute and the number of moles in that mass is determined.

Eq6

This text is adapted from Openstax, Chemistry 2e, Section 11.4: Colligative Properties.

Suggested Reading

  1. Steffel, Margaret J. "Raoult's law: A general chemistry experiment." Journal of Chemical Education 60, no. 6 (1983): 500.
  2. Berka, Ladislav H., and Nicholas Kildahl. "Experiments for Modern Introductory Chemistry: Intermolecular Forces and Raoult's Law." Journal of chemical education 71, no. 7 (1994): 613.