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Fall 2009 |
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| Exercise: Colligative Properties of Solutions |
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Discussion Modules |
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Remember that Colligative properties depend only on the number or concentration of particles in a solution. The properties are, for ideal solutions, independent of the kind or size of the particles, whether ionic, large or small etc. As a consequence:
In these exercises we will be using the equations for the various colligative properties we have studied:
Recall also the definitions of the three concentration measures fundamental to solution colligative behaviors:
For a vapor pressure problem we will use the Raoult's Law equation, P = XP°
First we need to ask ourselves if the solute is covalent (moles of particles = moles) or ionic (moles of particles = moles of ions). In this case all of the atoms are hi or intermediate, so can consider covalent.
Next we need to determine the number of moles of each:
- MWacetone = 3(12.01) + 6(1.008) + 16.00 = 58.1 g/mol; Molesacetone = 10.00g/58.1g mol-1 = 0.172 mol.
- Molessulfanilamide = 1.00g/172.1g mol-1 = 5.81 x 10-3mol.
We can now find the mole fraction of acetone, Xacetone = 0.172mol/(0.172 mol + 5.81 x 10-3mol) = 0.967
Finally, P = XP° = (0.967)(4.00 x 103mmHg)
P= 3.87 x 103mmHg
Both of these substances are organic solvents, so covalent (the vapor pressures give away that they are not ionic since ions do not vaporize at normal temperatures).
Since the concentrations add up to 1.000 m we can use their concentrations as their mole fractions (e.g. 0.600/1.000 = 0.600)
Let's then find the vapor pressures of each solvent individually:
Ptoluene = XtolueneP°toluene = (0.600)(139 mmHg) = 83.4 mmHg
Pbenzene = XbenzeneP°benzene = (0400)(392 mmHg) = 157 mmHg
Recalling Dalton's Law of partial pressures, Ptotal = Ptoluene + Pbenzene = 83.4 mmHg + 157 mmHg
Ptotal= 2.40 x 102mmHg
Reading the problem this appears to be a boiling point elevation problem, so
Tb = K bm
First we need to find the concentration in molality.
- The data given allow us to find moles/g and kg
- molesurea = 0.300g/60.1g mol-1 = 4.99 x 10-3 moles
- kgwater = (10.0g)(1 kg/1,000g) = 0.0100 kg
- molality can then be found by conversion to kg: molality = (4.99 x 10-3 moles)/(0.0100 kg) = 0.499 m
and,
Tb = K bm
Tb = (0.512 °C m-1)(0.499 m) = 0.256°C
Finally, we can add the boiling point elevation to the boiling point of pure water at 1 atm, 100.00°C,
T = 100.256°C = 100.26°C
Reading the problem this appears to be a boiling point elevation problem, so
Tb = K bm
Because benzene is a non-polar solvent we know the unknown is NOT ionic, since ionic compounds will not dissolve in non-polar solvents.
In this case we can use the equation to find the molality, which in turn we can use to find moles and thus molecular weight.
Rearranging, m = (
Tb)/(K b); m = (82.6 - 80.2 °C)/(2.52 °C m-1) = (2.4°C)/(2.52 °C m-1) = 0.95 m 0.95 mol/kg
And from the grams we find that (7.39g/[85.0g][1kg/1,000g]) = (7.39g)/(0.085kg) = 86.9 g/kg
Finally,
MW = (86.9 g/kg)/(0.95 mol/kg) = 91g/mol
Reading the problem this appears to be a boiling point elevation problem, so
Tb = K bm
Writing out the formula of the compound by consulting the Periodic table we get, FeCl3 which we expect to be ionic (Fe is lo, Cl is hi).
As a result we see that we will have four moles of ions per mole of substance, so our molality, m = 4(0.250 m) = 1.00 m
The boiling point increase is then
Tb = K bm = (0.512 °C m-1)(1.00 m) = 0.512°C.
Adding the boiling point increase to the boiling point of water at 1.00 atm we get:
T = 100.512°C = 100.51°C
From reading the problem this is a freezing point depression problem and
Tf = -Kfm
In this case we can use the equation to find the molality, which in turn we can use to find moles and thus molecular weight.
Rearranging, m = (
Tf )/(-Kf) = (1.96°C)/(5.12 °C m-1) = 0.383 m = 0.383 mol/kg solv.
Now if we find the mass/kg solv. we can find the molecular weight: 1.42g/0.025kg = 56.8g/kg solv.
Finally:
MW = (56.8g/kg solv.)/(0.383 mol/kg solv.) = 148g/mol
Reading the problem this appears to be a freezing point depression problem and
Tf = -Kfm
Writing out the formula of the compound by consulting the Periodic table we get, AlCl3 which we expect to be ionic (Al is lo, Cl is hi).
As a result we see that we will have four moles of ions per mole of substance, so our molality, m = 4(0.100 m) = 0.400 m
The freezing point depression is then:
Tf = -Kfm = (-1.988°C m-1)(0.400 m) = -0.7952 °C
So the freezing point becomes 0.000 -7.952 °C
Tf = -0.795°C
For this problem we want to recall that acetic acid is a weak acid, so the molality will be the sum of the acid plus the hydrogen ion and acetate ion concentrations.
From the data we can find the total molality. Rearranging the freezing point depression equation,
Tf = -Kfm, we get: m = (
Tf )/(-Kf)
Solving with the data provided, m = (-0.28°C)/(1.855 °C m-1) = 0.1509m
In this case we started by adding 0.150 moles of acetic acid, which then partially dissociated.
CH3COOH
CH3COO-1 + H+1
So after dissociation, assuming x is the amount dissociated we have:
- acetic acid = 0.150 - x
- acetate ion = x
- hydrogen ion = x
- total moles then = 0.150 - x + 2x = 0.150 + x
Thus hydrogen ion concentration, [H+] = x = 0.1509m- 0.150m= 0.009m
[H+] = 0.009m
= MRT
Of course sodiium chloride is ionic so the molarity of ions is double the stated molarity, 2(0.500 M) = 1.000 M = 1.000 mol L-1
Plugging values into the equation we get
= (1.000 mol L-1)(0.0821 L atm mol-1 K-1)(273.15 K)
= 22.4atm
= MRT
To find the molecular weight we need to have moles and grams. We are given grams in the problem, so first let's find the moles via finding M
Rearranging the osmotic pressure equation we get M =
/RT. Substituting values then we get:
M = {(1.35 mmHg)/(760 mmHg atm-1)}/{(0.0821 L atm mol-1 K-1)(273.15 +25)K = (1.78 x 10-3 atm)/{(0.0821 L atm mol-1 K-1)(278 K)}
M = 7.275 x 10-5 mol/L
From the problem we see that the solution had 0.500 g/100.0 mL = 5.00g/L
To get g/mol we then can use dimensional analysis to set up the equation:
MW = (5.00 g/L)/(7.275 x 10-5 mol/L) = 6.87 x 104g/mol
In addition to these exercises you should familiarize yourself with the text materials.
© R A Paselk
Last modified 7 November 2009