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Figure 6.13. Order parameter vs. reduced concentration of lyotropic liquid crystalline
polymers. (From Doi & Edwards, 1986.)
1
4
of the reduced concentration φ/φ =
8
9
and then gradually approaches
unity.
Lee (1988) further connected the viscosities of liquid crystalline polymers
(in the unit of η ) with concentration and molecular length as Equa-
tion (6.37), where λ is a constant less than unity which is associated with
the stability of simple shear flow, µ is a dimensionless parameter associ-
ated with the interaction in the fluid, R =
P 4 (
a · n
)
is the second order
parameter where
is the molecular long axis and P 4 is the fourth rank
Legendre polynomial.
a
α 1 =
(2
µ ) R,
1+ 1
λ
S,
α 2 =
1
S,
(6.37)
1
λ
α 3 =
α 4 = 2
105
[7(3 + µ )
5(3+2 µ ) S
3(2
µ ) R ] ,
 
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