2. Solubility and Molecular Weights

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Experimental Method:
Determination of : Osmotic Pressure
 1      V1
0
1
V1  Molar Volume
of the Solvent

0
2
(  1   1 )    V1  RT ln( 1  v 2 )  v 2 (1  1 )   v 2
x

ln( 1  v 2 )   v 2  v / 2
2
2
V 1
RT
1


 v 2      v 2  1 / x 
Polymer
 Solubility 
2
1
The osmotic
pressure data for
cellulose tricaproate
in
dimethylformamide
at three
temperatures. The
Flory temperature was
determined to be 41
± 1°C
 
1
2
 A 2V1 
2
2
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2
Modified Flory-Huggins theory
 Is temperature dependent
  Hmix 
2  

   RT 
N


 T
 S Mix
N

 v1 v 2


  T   
  R  n1 ln v1  n 2 ln v 2  v1 v 2 
 
 T  

Therefore, any temperature which causes =1/2 will
be the Flory  temperature
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3
Flory-Huggins Parameters
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4
An Example
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5
Applications of 
The Chain Expansion Ratio and -Temperature
The Expansion Ratio, r
r 
2
r
r
2
2
o
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6
Applications of 

r depends on balance between i) polymer-solvent and ii) polymerpolymer interactions

If (ii) are more favourable than (i)
 r < 1
 Chains contract
 Solvent is poor

If (ii) are less favourable than (i)
 r > 1
 Chains expand
 Solvent is good

If these interactions are equivalent, we have theta condition


r = 1
Same as in amorphous melt
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7
Applications of 


For most polymer solutions r depends on temperature, and
increases with increasing temperature
At temperatures above some theta temperature, the solvent is good,
whereas below the solvent is poor, i.e.,
T>q
r > 1
T=q
r = 1
T<q
r < 1
Often polymers will precipitate
out of solution, rather than contracting
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8
Applications of 
The Solvent Goodness:
A2  (
•
•
•
•
1
2
  )(
1
V1 
2
2
)
A Positive A2 indicates a good solvent, i.e. a solvent that gives rise to
an exothermic enthalpy of mixing. This arise when <1/2.
When A2=0 the solvent is nearly Ideal. This is important for use of
osmotic pressure to measure molar mass.
A negative A2 indicates a poor solvent (>1/2). The entalpy of mixing is
positive here.
The goodness of solvent can be adjusted by changing the temperature.
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9
Applications of 
Recall:
 H mix  RT  1 N 1v 2
 1  z  w12 / RT
 w12  2 ( w11 w12 )
1
2
 w11  w 22  ( w11 )
1/ 2
 ( w 22 )
1/ 2
Note that the energy terms w11, w22 and w12 are attractive
terms and are usually negative .
When Hmix =0 for a solvent -polymer system, thus w11=w22 and
the cohesive energy density.
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10
Summary
Solubility Parameters:
Thermodynamics of Mixing
 G Mix   H Mix  T  S Mix
 H Mix   kTN 1v 2
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11
Summary
Free Energy of Mixing:
   G Mix
 1    
  n1
0
1



 T ,P ,n2

2
1
(  1   )  RT ln( 1  v 2 )  v 2 (1 
)  v2
x
0
1
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
12
Summary
Chemical Potential and Osmotic Pressure:
 1      V1
0
1
V 1
RT
1

 v 2      v 2  1 /

2
A2  (
1
2
  )(

x 

1
V1 
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2
2
)
13
Summary
Other Forms of Flory-Huggins Eqs:
0.35 (in older literature), or zero
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14
Properties of 




If the value of  is below 0.5, the polymer should be
soluble if amorphous and linear.
When  equals 0.5, as in the case of the polystyrene–
cyclohexane system at 34°C, then the Flory 
conditions exist.
If the polymer is crystalline, as in the case of
polyethylene, it must be heated to near its melting
temperature, so that the total free energy of melting
plus dissolving is negative.
For very many nonpolar polymer–solvent systems,  is
in the range of 0.3 to 0.4.
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Properties of 



For many systems,  has been found to
increase with polymer concentration and
decrease with temperature with a
dependence that is approximately linear
with, but in general not proportional to, 1/T.
For a given volume fraction 2 of polymer,
the smaller the value of , the greater the
rate at which the free energy of the solution
decreases with the addition of solvent.
Negative values of  often indicate strong
polar attractions between polymer and
solvent.
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16
Properties of 

The polymer–solvent interaction
parameter is only slightly sensitive to the
molecular weight.
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17
Molecular Weight Averages
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18
Molecular Weight Distribution
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19
Determination of Number Average
Mw
a) End-group Analysis
b) Colligative Properties
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Osmotic Pressure
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Flory q-Temperature
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Intrinsic Viscosity
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Some Definitions
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The Mark-Houwink Relationship
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Experimental Techniques
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Example
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Example (cont.)
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Gel Permiation Chromatography
Size Exclusion Chromatography
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Schematic View
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Calibration
GPC is a relative Molecular Weight
Method
 Narrow molecular weight distribution,
anionically polymerized polystyrenes are
used most often.
 Other Polymers: PMMA, Polyisoprene,
polybutadiene, Poly(ethylene oxide) and
sodium salts of PMA.

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Calibration Method
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Molecular Weight of a Suspension
Polymerized PS
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GPC of a Blend
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End of Chapter 2
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