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(b) Solubility parameters of polymers (MPa) 1/2
Polymer b
H-bonding group c
δ
Polybutadiene
17.2
Poor
Polyisoprene
17.4
Poor
Poly(butadiene-co-styrene) 75/25
17.4
Poor
Poly(tetramethylene oxide)
17.6
Medium
Poly(butyl methacrylate)
18.0
Poor?
Polystyrene
18.4
Poor
Poly(methyl methacrylate)
19.0
Medium
Poly(butadiene-co-acrylonitrile) 75/25
19.2
Poor
Poly(ethyl acrylate)
19.2
Medium
Poly(vinyl acetate)
19.7
Medium
Poly(vinyl chloride)
19.9
Medium
Poly(methyl acrylate)
20.7
Medium
Polyformaldehyde
20.9
Medium
Ethyl cellulose
21.1
Strong
Poly(vinyl chloride-co-vinyl acetate) 87/13
21.7
Medium
Cellulose diacetate
23.3
Strong
Poly(vinyl alcohol)
26.0
Strong
Polyacrylonitrile
26.0
Poor
Nylon-6,6
28.0
Strong
a Selected data from Ref. [6] .
b Compositions of copolymers are in parts by weight.
c The hydrogen-bonding group of each polymer has been taken as equivalent to that of the parent
monomer. (The hydrogen-bonding tendency can be assigned qualitatively in the order alcohols .
ethers . ketones . aldehydes . esters . hydrocarbons or semiquantitatively from infrared
absorption shifts of CH 3 OD in a reference solvent and in the liquid of interest [7] .)
5.2.2 Flory
Huggins Theory
Nonideal thermodynamic behavior has been observed with polymer solutions in
which
H m is practically zero. Such deviations must be due to the occurrence of
a nonideal entropy, and the first attempts to calculate the entropy change when
long chain molecules are mixed with small molecules were due to Flory [8] and
Huggins [9] . Modifications and improvements have been made to the original the-
ory, but none of these variations has made enough impact on practical problems
of polymer compatibility to occupy us here.
The Flory
Δ
Huggins model uses a simple lattice representation for the polymer
solution and calculates the total number of ways the lattice can be occupied by
small molecules and by connected polymer segments. Each lattice site accounts
for a solvent molecule or a polymer segment with the same volume as a solvent
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