Local Structure and Elasticity of Soft Gelatin Gels Studied
with Atomic Force Microscopy
V. I. Uricanu,*
,†
M. H. G. Duits,
†
R. M. F. Nelissen,
†
M. L. Bennink,
‡
and
J. Mellema
†
Physics of Complex Fluids Group and Biophysical Techniques Group, Faculty of Science and
Technology, Associated with the J. M. Burgerscentrum for Fluid Mechanics, and Institute of
Mechanics, Processes and ControlsTwente (IMPACT), University of Twente, Postbus 217,
7500 AE Enschede, The Netherlands
Received April 24, 2003. In Final Form: July 8, 2003
Atomic force microscopy (AFM) measurements were done on aqueous gelatin gels submerged in dodecane.
Use of home-built AFM instrumentation coupled with dedicated analysis of the recorded force-displacement
curves, allowed the a posteriori extraction of both surface topography and elastic properties of these soft
samples. Hertz theory was used to obtain (apparent) relative Young moduli (E*) from the force-indentation
curves. For indentations smaller than 100 nm, scattered values of E* were found. This is partially attributed
to the structural inhomogeneity of the polymer network at these length scales. At larger indentations, the
relative Young moduli were found to be “compression-rate”-independent but to decrease with the indentation
depth (δ). This independence of the compression rate indicates quasi equilibrium elastic behavior (i.e., the
absence of stress relaxation by the gelatin), confirmed also by additional experiments, in which a truncated
sawtooth driving voltage was used. In these latter AFM recordings, the compression regime is combined
with a stationary piezo state when the AFM tip is in contact with the gel. The measured cantilever deflection
due to gel relaxation was always below 10% from the indentation depth. Additional features were observed
in the 3D recordings and associated with stiff fibrils lying on top of the soft gelatin network. Depending
on aging time and location along the sample surface, mobile single fibrils as well as tough, compact,
immobile fibril bundles were observed. A comparison was made between the relative Young moduli measured
with AFM and the elastic (storage) moduli as measured in a conventional rheometer. Taking as variable
the sample’s “age”, the microscopic and the macroscopic moduli turned out to be in good agreement in the
limit of high (polymer) concentrated gels. Gel syneresis, with water exudation from the 10% gelatin network,
was found to drastically increase the E* values found with AFM (at δ ) 250 nm). The fact that this was
not found with conventional rheometry might suggest a different syneresis behavior in dodecane.
Introduction
Gelatin is an abundant and relatively inexpensive
protein derived from collagen, with the capacity to form
network structures and gels. It is used in a variety of gel
applications including photography, drug delivery, ho-
lography, microencapsulation, and food preparation.
Gelatin is also a promising structural biomaterial since
it does not show antigenity and toxicity and can be
completely resorbed in vivo. Its physicochemical properties
can be suitably modulated and its mechanical properties
can be improved and adjusted
2-5
by mixing gelatin with
inorganic
1,6-8
materials or with other natural and synthetic
polymers.
9-17
In native state, gelatin molecules are soluble in water
at 40-45 °C, where the individual chains act like
semiflexible coils. When the temperature drops below the
gelation limit (which is around 30-35 °C, depending on
the gelatin type and concentration), the initial solution
undergoes a sol-gel transition. The molecules rearrange
themselves in an attempt to adopt more energetically
favorable conformations; the most favorable one is the
triple-helix collagen structure.
18
However, due to simple
entanglements between gelatin macromolecules in solu-
tion, total re-formation of a compact collagen three-
dimensional network is not possible. In time, the triple-
helix regions propagate, can even aggregate, and generate
a coarse network that grows within the “fine” molecular
network of the simple entangled molecules. The formation
of triple-helixes starts immediately after the molecules
have come in contact at or below the gelation temperature
and continues indefinitely long after the initial setting of
* To whom correspondence should be addressed.
E-mail: v.i.uricanu@utwente.nl.
†
Physics of Complex Fluids Group.
‡
Biophysical Techniques Group.
(1) Bigi, A.; Panzavolta, S.; Roveri, N. Biomaterials 1998, 19, 739.
(2) Maeda, T.; Motoyoshi, H. Jpn. J. Polym. Sci. Technol. 1996, 53,
155.
(3) Fakirov, S.; Sarac, Z.; Anbar, T.; Boz, B.; Bahar, I.; Evstatiev, M.;
Apostolov, A. A.; Mark, J. E.; Kloczwski, A. Colloid Polym. Sci. 1996,
274, 334.
(4) Fakirov, S.; Sarac, Z.; Anbar, T.; Boz, B.; Bahar, I.; Evstatiev, M.;
Apostolov, A. A.; Mark, J. E.; Kloczwski, A. Colloid Polym. Sci. 1997,
275, 307.
(5) Zhao, W.; Kloczwski, A.; Mark, J. E.; Erman, B.; Bahar, I.
CHEMTECH 1996, 26, 32.
(6) Lin, F. H.; Yao, C. H.; Sun, J. S.; Liu, H. C.; Huang, C. W.
Biomaterials 1998, 19, 905.
(7) Wan, Y. Z.; Wang, Y. L.; Yao, K. D.; Cheng, G. X. J. Appl. Polym.
Sci. 2000, 75, 994.
(8) Zheng, J. P.; Li, P.; Ma, Y. L.; Yao, K. D. J. Appl. Polym. Sci. 2002,
86, 1189.
(9) Yao, K. D.; Liu, W. G.; Lin, Z.; Qiu, X. H. Polym. Int. 1999, 48,
794.
(10) Jiang, H. L.; Zhu, K. J. J. Appl. Polym. Sci. 2001, 80, 1416.
(11) Kasapis, S.; Morris, E. R.; Norton, I. T.; Clark, A. H. Carbohydr.
Polym. 1993, 21, 269.
(12) Loren, N.; Langton, M.; Hermansson, A. M. Food Hydrocolloids
1999, 13, 185.
(13) Normand, V.; Pudney, P. D. A.; Aymard, P.; Norton, I. T. J.
Appl. Polym. Sci. 2000, 77, 1465.
(14) Normand, V.; Plucknett, K. P.; Pomfret, S. J.; Ferdinando, D.;
Norton, I. T. J. Appl. Polym. Sci. 2001, 82, 124.
(15) Marrs, W. M. Prog. Food Nutr. Sci. 1982, 6, 259.
(16) Tromp, R. H.; Rennie, A. R.; Jones, R. A. Macromolecules 1995,
28, 4129.
(17) Vinches, C.; Parker, A.; Reed, W. F. Biopolymers 1997, 41 (6),
607.
8182 Langmuir 2003, 19, 8182-8194
10.1021/la0347004 CCC: $25.00 © 2003 American Chemical Society
Published on Web 08/29/2003