Table 2 Dielectric data at 50 uC and 1 kHz for formulations
containing polymers 4 and 5aa
Conclusions
We have reported the synthesis and characterization of a series
of new cyclo-copolymers containing unconventional crown
ethers embedded in their polymer chains. Even though they
incorporate a substantial portion of ethylene glycol units
(51 wt% for 4 and 56 wt% for 5a), their thermal properties are
substantially different from poly(ethylene glycols) since they do
not possess melting or glass transitions.
The new materials possess desirable film-forming character-
istics, and it was possible to prepare films in the micrometer
range by spin-coating. The conductivity of these films is not
yet enough to allow high-energy delivery (e.g. for lithium
batteries); however, the explored polymer architectures are of
interest because of the possibility to ‘tune’ their dimensions
and/or their order to allow new functional properties. Our
approach is indicative of how the molecular properties of the
recognition unit (i.e. crown ethers instead of open chain
glycols) cannot be discerned from their physical properties
(e.g. glass transition temperature). These new, robust polymers
could be useful in those applications of material science
requiring high thermal stability.
Samplea
e’
1.45
e@
s/V21 cm21
4
0.26
0.10
0.06
0.08
2.6 6 10211
2.6 6 10211
3.4 6 10211
4.1 6 10211
1.22 6 10210
1.31 6 10210
2.78 6 10210
6.91 6 10211
4.51 6 10210
4 1 Li (5:1)b
5a
1.60
2.78
3.35
2.68
9.45
15.32
2.83
7.45
5a 1 Li (5:1)b
5a 1 PEO
32.95
5a 1 PEO 1 Li (1:1)c
5a 1 PEO 1 Li (2:1)c
5a 1 PEO 1 Li (4:1)c
5a 1 PEO 1 Li (8:1)c
5020
109.7
32.4
74.65
a The ratio polymer/PEO is always 1:1 wt. b The amount of lithium
salt is expressed as the molar ratio obtained by considering the aver-
age molecular weight of the repeat monomer unit. c The amount of
lithium salt is expressed as the ratio between the moles of PEO and
those of the salt in the sample.
same sample doped with LiTFSI (PEO:LiTFSI 8:1). A plateau
giving the value of d.c. conductivity is observed at low
frequencies, followed by a dispersive behavior above 1 kHz,
which is probably related to the onset of slow re-orientational
motions of parts of the polymer backbone. Similar behaviors
are observed for all the other doped samples (see also Table 2).
The conductivity of the non-doped sample is likely due to
impurities introduced during the synthesis procedure (e.g.
Na1 ions) or to moisture. The addition of the lithium salt
causes only a minor change of the overall conductivity,
instead of the expected orders-of-magnitude increase which is
typical of salt-doped, PEO-based systems. This means that
the crown structures of the polymer 5a do not allow fast
diffusion of the lithium ions, and that the usual mechanisms
of conduction assisted by segmental motions, typical of
amorphous PEO–salt phases,13 are not effective. Therefore,
we can suppose that the highly regular structure of polymer
5a is able to hinder the growth of the amorphous phases
which are normally observed in PEO–salt systems near the
eutectics.
Table 2 reports the values of permittivity (e’), loss factor (e@)
and conductivity (s) at a specific frequency and temperature
for all the films we prepared. Generally speaking, we observe
that the addition of an ether group in order to increase
the amorphous fraction of the copolymer (sample 5a vs. 4)
does not practically affect the conductivity, whereas it makes
e’ change by a factor of two. On the other hand this result
may be somehow expected, since the added monomer contains
ethylene oxide groups, and it is well known from the
literature14 that the dielectric constant of amorphous PEO
is roughly twice that of the crystalline polymer. The addition
of PEO to both the polymers 4 and 5a determines an
orders-of-magnitude increase of the electric loss factor. As
far as concerns the transport properties, finally, the addition
of the lithium salt to the polymer blend does determine, at
most, a conductivity increase by a factor of two. Further
work is needed in order to prepare matrices allowing effective
ion transport. In particular, we stress that our chief aim in
this work was to see if highly ordered crown ether structures
could allow high lithium transport. As a consequence, the
addition of PEO was chiefly made to improve filmability and,
only as a ‘byproduct’, to add another mechanism for ion
motion.
Acknowledgements
We thank Dr Alessandro Galbiati (N.P.T. Polyurethane
Technologies, Gropello Cairoli, Italy) for performing the Gel
Permeation Chromatography analyses of the samples reported
here. Funding by the University of Pavia (FAR 2001-2003) is
acknowledged with thanks.
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In this frame, some developing strategies are: (i) changing the
crown ether dimension, (ii) changing the PEO MW (short chain
PEGs are recognized to work well in polymer electrolytes), and
(iii) adding plasticizers (e.g. ethylene carbonate). Another
important point in order to improve lithium transport is the
study of the relationships between crystallinity of the malonate
structures and ionic conductivity.
2 5 2 8
J . M a t e r . C h e m . , 2 0 0 4 , 1 4 , 2 5 2 4 – 2 5 2 9