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>> In this module we're talking
about colligative properties,
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specifically boiling
point elevation,
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freezing point depression,
and osmotic pressure.
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First of all, what a
colligative property is.
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It's a property of a solution
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that depends only upon how
many solute particles there are
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and not their identity.
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So, boiling point elevation.
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First of all, this is
the important equation
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that you're going to memorize.
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It says that the change
in the boiling point
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of a solvent is equal
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to something called the van't
Hoff factor times the molality
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of that solution, times the --
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what's called the boiling
point elevation constant.
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So, first of all, the
parts of this equation.
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The change in the boiling
point is the boiling point
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of the solution minus
the boiling point
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of the pure solvent,
before you add something in.
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Now, it ends up that
for any liquid,
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if you add a non-volatile
solute,
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you will increase
the boiling point,
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that's what this is
describing of that --
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of the resulting solution
compared to the pure solvent.
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Because, this number's
always bigger than this,
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this will always be
a positive number.
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This i, the van't Hoff
factor, this is the definition,
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it's the mols of particles
in the solution divided
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by the mols of the solute.
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If it's a molecular
compound, then i ,
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the van't Hoff factor is just
1, because for every particle
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for that molecular --
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that molecule you put in
there you just get, you know,
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it's the same particle inside.
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However, if it's
an ionic compound,
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then it can dissociate
in that solution.
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And when it does, you
create more particles.
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For example, if you put
sodium chloride into water,
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it dissociates into sodium
ions and chloride ions.
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So, it would be about 2 over 1.
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So, 1 -- for every 1
mol of sodium chloride,
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we get about two mols
of particles roughly.
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Come back to that in a second.
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Molality is the same
as we saw before.
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Remember the definition
of molality,
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it's mols of solute divided
by kilograms of solvent.
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And this boiling point elevation
constant, you look it up,
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you don't have to
memorize any of them.
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Just, the only thing -- the
important thing to remember is
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that you look it up based upon
what the solvent is, that's all.
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So, this van't Hoff factor.
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So, like we were saying,
if it's sodium chloride,
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we'd expect one formula unit
of sodium chloride to break
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up into two particles, the
sodium ion and the chloride ion,
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we'd expect it to be -- the
van't Hoff factor to be 2.0.
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In fact, it's about 1.9.
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The reason for this is
something called ion pairing.
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So, when we put that sodium
ion in the water, okay,
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most of the sodium ions and
the chloride ions separate
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from each other, and
they're surrounded by a sea
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of solvation by water molecules.
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However, some of
them still say --
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stay associated with each other.
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And that means instead
of getting two particles,
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this whole thing here only
counts as one particle.
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Magnesium chloride, we'd
expect to get three particles,
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two chloride and one magnesium.
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So, we'd expect that
van't Hoff factor
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to be three, in fact it's 2.7.
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And here, just for
comparison notice that glucose,
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which is a molecular
compound does not dissociate.
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So, we'd expect it's
van't Hoff factor
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to be 1, and it actually is.
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So, freezing point
depression works
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like boiling point elevation,
except that the freezing point
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of a solution is always
lower than the freezing point
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of the pure solvent when you
add a non-volatile solute to it.
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So, here delta T F, the change
in freezing point is equal
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to the freezing point
of the solution,
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minus the freezing point of
the solvent -- pure solvent.
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Now, because this would
be lower than this,
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this will be a negative
number delta T F.
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When you're putting it here
in this equation to use it,
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just make it positive, it'll
work out better that way.
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Same van't Hoff factor,
same volatility.
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The freezing point
depression constant,
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again it depends only
upon what the solvent is.
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You look it up, you don't
have to memorize any of them.
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So, why does this happen?
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Well this is a Phase
diagram for water.
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Please pardon my attempt
to draw curves here.
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But, the idea is this, we
know from the last module
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that by adding a solute
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to a solvent we lower
the vapor pressure
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of the resulting solution.
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And so, in this Phase diagram,
remember it's solid over here,
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it's liquid here, and
its gas over here.
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So, this is pressure
versus temperature.
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As we go along this curve,
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the pressure along this curve
here will be the vapor pressure
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of that liquid, in
this case water.
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So, by adding -- so, we know
by adding the solute we go
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over the vapor pressure.
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That's why the green curve
which it the vapor pressure
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of the solution, is lower
than the white curve,
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which is the vapor
pressure of pure water.
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So, green is the vapor
pressure of the solution,
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white is the vapor
pressure of water.
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And so, if we look at, okay,
this is one atmosphere,
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the pressure -- the
external pressure, right?
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Let's say that the atmospheric
pressure was one atmosphere.
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The solution or the
solvent will boil
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when its vapor pressure is
equal to the external pressure.
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So, when the vapor pressure
reaches one atmosphere,
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that temperature is
the boiling point.
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Because this is -- this curve
is higher than this curve,
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we reach that point at a lower
temperature for the pure solvent
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than we do for the solution.
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This difference here is the
change in the boiling point --
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the boiling point elevation
going from here pure solvent
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to here , the solution
Same thing works
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with the freezing point,
only the opposite way.
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This is a temperature at which,
you go from liquid to solid
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or solid to liquid,
the freezing point.
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So, from pure solvent,
in this case water,
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it would be this
temperature right here.
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The lowering of the vapor
pressure of the solution means
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that it freezes at a
lower temperature here.
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And this difference
here would be the change
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in the freezing point.
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Now, we -- remember
when we talked
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about vapor pressure lowering
by an addition of the solute.
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We -- and talked about
how entropy is involved,
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it still applies here,
it's the same reasoning.
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All right.
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So, the other colligative
property is osmotic pressure.
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This is supposed to be a
pi, we call it pi capital.
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And osmotic pressure is equal
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to the van't Hoff
factor, same as before.
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Now this M is the
Molarity not the molality,
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watch out it's a capital M,
times the gas law constant,
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which we know from before
from the gas factor.
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And T is the temperature
in kelvin.
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R, remember is .08206 liters
atmospheres per kelvin mol.
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And that's only four sig figs.
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So, what is osmotic pressure?
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Well, it ends up if you put
a solution and separate it
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from some of its solvent
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by what's called a
semi-permeable membrane,
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the column of liquid on the
side of the solution will rise,
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and -- but you can
stop it from rising
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by exerting an --
a pressure on it.
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And that pressure for that
solution is the osmotic pressure
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of that solution.
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So, if we look at it, this --
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what this semi-permeable
solution does is it allows
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solvent particles
to pass through
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but not solute particles.
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So, what the -- what'll here
is just left to its own,
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the pure solvent
side is going to try
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to dilute the solution side.
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And it's -- what
it's trying to do is
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to get the concentration the
same on both sides, zero,
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it can never get there.
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But what happens is, as
the solvent particles pass
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through the semi-permeable
membrane,
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this column of liquid
starts increasing in height.
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And just like with the
mercury barometer we talked
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about in the gas chapter,
as it increases --
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as it goes up higher and
higher in this column,
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gravity is exerting
a force down,
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and thus creating a
pressure at this barrier.
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And when it reaches a height
such that the pressure exerted
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down balances the pressure
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of the solvent coming
through, it stops rising.
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That difference is a measure
of the osmotic pressure.
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So, let's do an example.
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This one happens to deal with
freezing point depression,
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but boiling point elevation
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and osmotic pressure
calculations are pretty similar,
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just remember those equations.
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So, we have 1 gram of quinine
-- quinine, it's a molecule,
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a molecular compound,
is dissolved
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in 10 grams of cyclohexane.
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So, quinine is a
molecular compound
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as is cyclohexane an enzyme.
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The freezing point
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of the resulting solution
is .24 degrees Celsius,
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almost 0 not quite.
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What's the normal
mass of quinine?
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If we have pure cyclohexane
it ends up that it freezes
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at 6.47 degrees Celsius.
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And the freezing point
depression constant
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for the solvent which
is cyclohexane is this,
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20.2 kelvins per molal.
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So, here our approach
is going to be,
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we're going to use the freezing
point depression equation.
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And we're going to solve
it for the molality.
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Because -- okay, so, the freeze
-- first the freezing point,
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it's the freezing point
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of the solution minus
the freezing point
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of the pure solid.
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Which is, .24 minus
6.47 degrees,
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it's negative 6.23
degrees Celsius.
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And because, the
difference in the temperature
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in Celsius is the same as
the difference in kelvin,
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this is also the difference
in the freezing point,
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the change in the freezing point
is also negative 6.23 Kelvin.
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Think about that if
you're not sure why
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that is, but that's true.
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And so, now we have the freezing
point depression equation,
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we're going to solve
for the molality.
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Here, because quinine is a
molecular compound, i is 1.
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So, we don't have
to worry about it.
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If we solve for the molality,
just divide the change
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in freezing point, we're going
to make it positive, by the,
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well i, the van't Hoff factor
times the freezing point
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depression constant, i is 1.
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We saw that k is
-- k sub F is 20.2,
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I gave you that T
in the problem.
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Do the division, we get
.308, three sig figs,
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first insignificant
figure is a 4, molality.
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So, that's the molality
of the solution But,
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we want the molar
mass of the quinine.
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So, what we're going to do
is, because the definition
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of molality is mols of solute
over kilograms of solvent.
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And we know how many kilograms
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of solvent, which
is cyclohexane.
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We had 10.0 grams, which
is 0.1000 kilograms --
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two zeros after that.
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If we multiply the molality
that we just figured
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out times the kilograms of
solvent, we get mols of solute.
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So, this is mols of
quinine, the solute.
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And all we have to do now to get
the molar mass is take the mass
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of the quinine in grams divided
by the mols, grams per mol.
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So, the molality was 1 gram
divided by that many mols.
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When we do the division
we get to three sig figs,
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and you are 3.24 grams per mol.
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And there you go.