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Chem102ColligativeProperties

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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.
Title:
Chem102ColligativeProperties
Description:

Colligative properties of solutions: boiling point elevation, freezing point depression, and osmotic pressure.

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Video Language:
English
Duration:
11:19

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