solutions
DESCRIPTION
explain about solutionsTRANSCRIPT
Properties of Solutions
Concentration Terms
Dilute - not a lot of solute. Concentrated - a large amount of solute. Concentration can be expressed
quantitatively is many ways:• Molarity
• Molality
• Percentage
• Mole fraction
Molarity and Molality
The molarity is the number of moles of solute in 1 litre of solution.• M = moles of solute / V sol’n (litres)
The molality is the number of moles of solute in 1 kg of solvent.• M = moles of solute / kg solvent
Conversion between the two requires the solutions density.
Partial Molar Thermodynamic Properties
Define a partial molar thermodynamic property as
Euler’s Theorem
'n,P,TJJ n
YY
J
JJYnY
The Chemical Potential
We define the chemical potential of a substance as
'n,P,TJJ n
G
The Wider Significance of
Shows how all the extensive thermodynamic properties depend on system composition
'n,V,SJJ n
U
'n,P,SJJ n
H
'n,V,TJJ n
A
Thermodynamics of Mixing
Spontaneous mixing of two or more substances to form solutions
Gibbs energy of the solution must be less than G(pure components)
The Gibbs Energy of Mixing
J
JJmix XlnXnRTG
The Enthalpy and Entropy
lnmixJ J
JP
mix
GnR X X
T
S
2
mixmix
P
GHT
T T
The Ideal Solution
TmixS/n
TmixG/n
TmixH/n0
kJ/mol
XA
The Volume and Internal Energy of Mixing
VPG
mixT
mix
VPHU mixmixmix
Ideal Solution Def’n
For an ideal solution
0H;0V mixmix
0
VPHU mixmixmix
Raoult’s Law
Consider the following system
Raoult’s Law #2
The chemical potential expressions
AO
AA
A*AA
plnRTvapvap
XlnRTliqliq
Raoult’s Law: Depression of Vapour pressure
VP of solution relates to VP of pure solvent
PA = XAP*A
Solutions that obey Raoult’s law are called ideal solutions.
Raoult’s Law Example
The total vapour pressure and partial vapour pressures of an ideal binary mixture
Dependence of the vp on mole fractions of the components.
An Ideal Solution
Benzene and toluene behave almost ideally
Follow Raoult’s Law over the entire composition range.
Henry’s Law
Henry’s law relates the vapour pressure of the solute above an ideally dilute solution to composition.
The Ideal Dilute Solution
Ideal Dilute Solution• Solvent obeys
Raoult’s Law
• Solute obeys Henry’s Law
Henry’s Law #2
The chemical potential expressions
JO(H)
is the Henry’s law standard state.
It is the chemical potential of J in the vapour when PJ = kJ.
( )' ln
ln
O HJ J J
OJ J J
sol n liq RT X
vap vap RT p
Henry’s Law #3
The Standard State Chemical potential for Henry’s Law
When the system is in equilibrium
The chemical potential expressions reduce to Henry’s Law
J
oJ
oH,J
klnRT
vap
vapn'sol JJ
JJJ XkP
Henry’s Law in terms of molalities
The Standard State Chemical potential for Henry’s Law
When the system is in equilibrium
The chemical potential expressions reduce to Henry’s Law in terms of molalities
oJoHJ
omJ mMRT ln,,
vapn'sol JJ
J
mJJ mkP
Chemical Potentials in terms of the Molality
The chemical potential expressions
o
JmJJ m
mRTnsol ln' ,
oJ,m = chemical potential of the solute in an
ideal 1 molal solution
The Gibbs-Duhem Equation
The Gibbs-Duhem gives us an interrelationship amongst all partial molar quantities in a mixture
J
JJdYn0
Colligative Properties
Colligative Properties
All colligative properties• Depend on the number and not the nature
of the solute molecules Due to reduction in chemical potential
in solution vs. that of the pure solvent• Freezing point depression
• Boiling Point Elevation
• Osmotic Pressure
Boiling Point Elevation
Examine the chemical potential expressions involved
vapliq JJ
J*JJ XlnRTliqvap
G
XRTliqvap
vap
JJJ
ln*
Boiling Point Elevation #2
The boiling point elevation
B
vap
bb X
JHJRT
T2
*
BbJvap
Jbb mKm
JHMRT
T2
*
Freezing Point Depression
Examine the chemical potential expressions involved
sliq *JJ
J*JJ XlnRTliqliq
G
XlnRTliqs
fus
J*J
*J
Freezing Point Depression #2
Define the freezing point depression
B
fus
ff X
JHJRT
T2
*
BfJ
fus
ff mKm
JHJMRT
T2
*
Osmosis
Osmosis
The movement of water through a semi-permeable membrane from dilute side to concentrated side• the movement is such that the two sides
might end up with the same concentration
Osmotic pressure: the pressure required to prevent this movement
Osmosis – The Thermodynamic Formulation
Equilibrium is established across membrane under isothermal conditions
PP *JJ
J*JJJ XlnRTPX,P
- the osmotic pressure
The Final Equation
RTMRTVn
BB
The osmotic pressure is related to the solutions molarity as follows
Terminology
Isotonic: having the same osmotic pressure
Hypertonic: having a higher osmotic pressure
Hypotonic: having a lower osmotic pressure
Terminology #2
Hemolysis: the process that ruptures a cell placed in a solution that is hypotonic to the cell’s fluid
Crenation: the opposite effect
The Partial Molar Volume
In a multicomponent system
J
JJVnV
'n,P,TJJ n
VV
Volume Vs. Composition
The partial molar volume of a substance • slope of the variation of the
total sample volume plotted against composition.
PMV’s vary with solution composition
The PMV-Composition Plot
The partial molar volumes of water and ethanol at 25C.
Note the position of the maxima and minima!!
Experimental Determination of PMV’s
Obtain the densities of systems as a function of composition
Inverse of density – specific volume of solution
mLg1
gmLVs
2CmBmAmolmLV
Example with Methanol.
Plot volumes vs. mole fraction of component A or B
Draw a tangent line to the plot of volume vs. mole fraction.
Where the tangent line intersects the axis – partial molar volume of the components at that composition
The Solution Volume vs. Composition
The Mean Molar Volume
Define the mean mixing molar volume as
• V*J – the molar
volume of the pure liquid
• Vm = V/nT
J
*JJmmix VxVV
The Mean Molar Volume Plot
-1.20
-1.00
-0.80
-0.60
-0.40
-0.20
0.00
0.20
0.00 0.50 1.00
XMeOH
m
ixV
m /
(m
L/m
ol)
VA-VA* VB-VB
*
Infinite Dilution Partial Molar Properties
The value of a partial molar thermodynamic property in the limit of zero volume is its infinite dilution value• E.g., for the volumes
J0xJ VlimVJ
The Definition of the Activity
For any real system, the chemical potential for the solute (or solvent) is given by
Jo
J aRT ln
Activities of Pure Solids/Liquids
The chemical potential is essentially invariant with pressure for condensed phases
ooJ
p
P
Joo
JJ
P
dpVPPo
Pure Solids and Pure Liquids
For a pure solid or a pure liquid at standard to moderately high pressures
JaRT0 ln
or aJ = 1
Activities in Gaseous Systems
The chemical potential of a real gas is written in terms of its fugacity
Jo
J fRT ln
Define the Activity Coefficient
The activity coefficient (J) relates the activity to the concentration terms of interest.
In gaseous systems, we relate the fugacity (or activity) to the ideal pressure of the gas via
JJJ fP
Activities in Solutions
Two conventions Convention I
• Raoult’s Law is applied to both solute and solvent
Convention II• Raoult’s Law is applied to the solvent;
Henry’s Law is applied to the solute
Convention I
We substitute the activity of the solute and solvent into our expressions for Raoult’s Law
*J
IJJ PaP
IJJ
IJ ax
Convention I (cont’d)
Vapour pressure above real solutions is related to its liquid phase mole fraction and the activity coefficient
*JJ
IJJ PxP
Note – as XJ 1J
I 1 and PJ PJid
Convention II
The solvent is treated in the same manner as for Convention I
For the solute, substitute the solute activity into our Henry’s Law expression
JIIJJ kaP
IIJJ
IIJ ax
Convention II (cont’d)
Vapour pressure above real dilute solutions is related to its liquid phase mole fraction and activity coefficient
JJIIJJ kxP
Note – as XJ 0J
II 1 and PJ PJid
Convention II - Molalities
For the solute, we use the molality as our concentration scale
mJJ
mJ am
mJ
moJJ aRT ln
Note – as mJ 0J
(m) 1 and aJ(m) mJ