We study micellization for A–B diblock copolymers of length N
1 with
the volume fraction of the insoluble block f
B in A polymeric solvents of length N by dilute solution thermodynamics. For short-chain solvents,
the micelle is “wet”, and the critical micelle condition
is given by
false(
χ
N
false)
normalc
.
normalm
.
−
1
/
2
∼
(
f
B
N
1
)
−
1
/
2
N
1
/
2
with the optimal aggregation number at
the transition m
c.m.
* ∼ N
1/2
p
3/2 (p=b
2/v
0
2/3 is the stiffness
parameter), in agreement with the extended Lifshitz theory. However,
the micellization point for the “dry” micelle is
false(
χ
N
false)
normalc
.
normalm
.
−
1
/
2
∼
(
f
B
N
1
)
−
1
N
with
m
normalc
.
normalm
.
*
∼
(
f
B
N
1
)
1
/
2
p
3
/
2
in the long-chain solvents. A theoretical
analysis shows that the micellization point is a universal function
of the apparent scaling variable x
m ≡ N/f
B
N
1. Interestingly, on combining the scaling behavior of m
c.m.
*, (χN)c.m. shows a universal scaling behavior with an intrinsic scaling variable x ≡ (pN)3/2/m*f
B
N
1, which
has a clear physical meaning as the ratio between the pervaded volume
of the polymeric solvent and the physical volume of the micellar core.
In addition, after proper nondimensionalizing, the micelle density
profile and the interfacial thickness at the micellization point also
show universal behaviors with both x
m and x. Importantly, micelles with several to thousands of chains
show great potential for application in drug and gene delivery diagnostics,
nanoreactors, and microcapsules.