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of the crystal/vapour, crystal/substrate, amorphous/vapour, amorphous/substrate
and crystal/amorphous interfaces, respectively.
The first term in Eq. (5.11) reflects the gain in the bulk energy while the sec-
ond term accounts for the variation in the total free energy associated with the
replacement of the substrate/amorphous and vapour/amorphous interfaces (d A 1 )
by the substrate/crystal and vapour/crystal interfaces. The last term represents the
increase in the total free energy due to the increase in the crystal/amorphous in-
terface (d A 2 ). Taking into account Eq. (5.11) and the expressions for d V ,d A 1 and
d A 2 given above, d G
/
d N can be expressed as:
1
d G
d N =− µ 0 +
1
h ( t )
γ + γ ca d h
d R
+ γ ca
R ( t )
1
h ( t )
v
+ γ ca
h
=− µ 0 +
γ + γ ca
R ( t ) .
(5.12)
d R
/
d t
/
v
Taking into account that R ( t )
h ( t ) and that d R
d t
h , Eq. (5.12) can be
approximated by:
d N =− µ 0 + γ
1
d G
h ( t ) =− µ.
(5.13)
Combining Eqs. (5.10) and (5.13) we obtain:
µ 0 γ
h ( t )
K c
k B T
v R =
(5.14)
and defining
k B T and h c γ 0 , Eq. (5.9) is obtained. Note
that Eq. (5.9) is only valid for h ( t )
v
K c µ 0 /
h c . Finally, the mathematical expression for
R ( t ) can be derived from Eq. (5.9) by integration. In this case:
v t c ln t
t c
R ( t )
=
v
R ( t )d t
= v ( t
t c )
,
(5.15)
where t c is defined as t c
0. Figure 5.9 shows the fit to
the experimental points obtained with Eq. (5.15). The predicted curves fit well the
experimental points. The effects of non-linearity are more evident for the spherulites
forming first because the factor 1
h c
/v
h . Note that R ( t c )
=
/
h c
h is rather small, while for spherulites
appearing later h c / h
1, so that the velocity nearly reaches an asymptotic limit
and the growth is thus approximately constant. h c has been estimated from TMAFM
measurements as 35 nm. This value is of the same order as those found for thin
films of polymethine dye salts, h c
30 nm (Dahne, 1995), as previously discussed.
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