Influence of Adsorption Conditions on the Structure of
Polyelectrolyte Multilayers
Karsten Bu ¨ scher,
†,‡
Karlheinz Graf,
§
Heiko Ahrens,
†
and Christiane A. Helm*
,†
Angewandte Physik, Universita ¨ t Greifswald, Friedrich-Ludwig-Jahn-Str. 16,
D-17487 Greifswald, Germany, Institut fu ¨ r Physikalische Chemie, Universita ¨ t Mainz,
Jakob-Welder Weg 11, D-55099 Mainz, Germany, and Institut fu ¨ r Physikalische Chemie II,
Universita ¨ t Siegen, Adolf-Reichwein-Str., D-57068 Siegen, Germany
Received November 16, 2001. In Final Form: January 30, 2002
Polyelectrolyte adsorption onto an oppositely charged interface is determined by electrostatic and
secondary interactions. Since polyelectrolytes precipitate at elevated temperatures, the secondary
interactions are presumably temperature dependent. This idea is tested for poly(allylamine) hydrochloride/
polystyrene sulfonate (PAH/PSS) films adsorbed from aqueous KCl solution (high salt conditions) at
temperatures between 5 and 40 °C. KCl was chosen because the films were thicker than those obtained
from NaCl or CsCl solutions indicating strong specific binding between K and PSS. The film thickness
increases continuously with the adsorption temperature; the changes amount to 20-40%, depending on
salt conditions. Furthermore, the roughness is increased, up to a factor of 5. The latter is attributed to
the decreased percentage of strong electrostatic bonds within the polyelectrolyte multilayer. Another path
to increased roughening is using low-weight polymers with a contour length similar to the thickness of
a polycation/polyanion pair.
Introduction
Polyelectrolyte multilayers
1
formed by sequential ad-
sorption of alternating charged polyelectrolytes have been
investigated a lot in recent years.
2
With this technique,
layered polymeric multicomposites with nanometer con-
trol can be built very easily, even on rough or bent sur-
faces.
3,4
The buildup principle is based on electrostatic
interaction; during each adsorption step the surface charge
is reversed,
5-7
and thus the adsorption of an oppositely
charged polyion is possible again. Yet, the actual surface
coverage is also determined by secondary interactions
8
and steric repulsion.
9
The range of possible applications
of polyelectrolyte multilayers increased even further when
it was realized that not only long-chain molecules but any
adsorbed multi-ion such as nanocolloids
10,11
or proteins
12
can be incorporated in a polyelectrolyte multilayer.
However, the adsorption properties of polyelectrolytes
are only qualitatively understood. Experimental find-
ings
13,14
and theoretical predictions
15,16
obtained so far may
be summarized as follows: Polyelectrolyte adsorption in
general is driven by either electrostatic attraction between
the polyelectrolyte segments and the surface carrying
opposite charges or short-range attractive forces (van der
Waals, hydrophobic, hydrogen bonding, or specific forces),
8
leading in most cases to charge reversal. Entropic effects
such as counterion release from both the surface and the
polyelectrolyte chains
14
also promote polyelectrolyte ad-
sorption. Besides those short-ranged attractive forces, also
repulsive forces determine the polyelectrolyte conforma-
tion: a multi-ion approaching a surface of the same charge
experiences a strong and long-ranged electrostatic repul-
sion. The polyelectrolyte conformation resulting from this
short-ranged attraction and long-ranged repulsion is very
flat, corresponding to one or two chain diameters.
14,16
When
the substrate with the adsorbed film is removed from the
solution, the adsorbed layer remains on the surface
because of the pronounced adsorption/desorption hyster-
esis that is typical for multisegment adsorption.
17
For
polyelectrolyte multilayers, the flat, homogeneous ad-
sorption implies a small roughness of the film/air interface,
which is very convenient for a controlled polyelectrolyte
multilayer architecture.
The flat conformation of adsorbed polyelectrolytes is
very different from the coiled conformation (approaching
a few radii of gyration) of neutral polymers. For those, the
important parameters are polymer length, segment/
interface interaction, and the “polymer-solvent interac-
tion parameter w”.
18
w is calculated from three inter- and
intramolecular interaction energies: solvent-segment
(ǫ
12
), solvent-solvent (ǫ
11
), and segment-segment (ǫ
22
).
* To whom correspondence should be addressed. E-mail:
christiane.helm@physik.uni-greifswald.de.
†
Universita ¨ t Greifswald.
‡
Universita ¨ t Mainz.
§
Universita ¨ t Siegen.
(1) Decher, G. Science 1997, 277, 1232-1237.
(2) Arys, X.; Jonas, A. M.; Laschewsky, A.; Legas, R. Supramolecular
polyelectrolyte assemblies; Ciferri, A., Ed.; Marcel Dekker: New York,
1999.
(3) Fou, A. C.; Onitsuka, O.; Ferreira, M.; Rubner, M. F.; Hsieh, B.
R. Mater. Res. Soc. Symp. Proc. 1995, 369, 575-580.
(4) Donath, E.; Walter, D.; Shilov, V. N.; Knippel, E.; Budde, A.;
Lowack, K.; Helm, C. A.; Mo ¨hwald, H. Langmuir 1997, 13, 5294-5305.
(5) Lowack, K.; Helm, C. A. Macromolecules 1998, 31, 823-833.
(6) Bertrand, P.; Jonas, A.; Laschewksy, A.; Legras, R. Macromol.
Rapid Commun. 2000, 21, 319-348.
(7) Schlenoff, J. B.; Dubas, S. T. Macromolecules 2001, 34, 592-598.
(8) Clark, S. L.; Hammonds, B. Langmuir 2000, 16, 10206-10214.
(9) Gru ¨ newald, T.; Da ¨hne, L.; Helm, C. A. J. Phys. Chem. B 1998,
102, 4988-4993.
(10) Schmitt, J.; Decher, G.; Dressick, W. J.; Brandow, S. L.; Geer,
R. E.; Shashidar, R.; Calvert, J. M. Adv. Mater. 1997, 9, 61.
(11) Schmitt, J.; Ma ¨ chtle, P.; Eck, D.; Mo ¨hwald, H.; Helm, C. A.
Langmuir 1999, 15, 3256-3266.
(12) Lvov, Y.; Ariga, K.; Ichinose, I.; Kunitake, T. J. Am. Chem. Soc.
1995, 117, 6117-6123.
(13) Fleer, G. J.; Stuart, M. A. C.; Scheutjens, J. M. H. M.; Cosgrove,
T.; Vincent, B. Polymers at Interfaces; Chapman and Hall: London,
1993.
(14) Ahrens, H.; Baltes, H.; Schmitt, J.; Mo ¨hwald, H.; Helm, C. A.
Macromolecules 2001, 34, 4504-4512.
(15) Joanny, J. F. Eur. Phys. J. B 1999, 9, 117-122.
(16) Netz, R. R.; Joanny, J.-F. Macromolecules 1999, 32, 9013-9025.
(17) Cohen-Stuart, M. Polyelectrolytes on Solid Surfaces; Daillant,
J., Guenoun, P., Marques, C., Muller, P., Va ˆ n, J. T. T., Eds.; Editions
Frontie `res: Gif-sur-Yvette, France, 1996; pp 1-12.
(18) Evans, D. F.; Wennerstro ¨m, H. The Colloidal Domain: Where
Physics, Chemistry, Biology, and Technology Meet; VCH: New York,
1994.
3585 Langmuir 2002, 18, 3585-3591
10.1021/la011682m CCC: $22.00 © 2002 American Chemical Society
Published on Web 03/28/2002