Fractal Analysis of Flame-Synthesized Nanostructured
Silica and Titania Powders Using Small-Angle X-ray
Scattering
Jingyu Hyeon-Lee,
†
Gregory Beaucage,*
,†
Sotiris E. Pratsinis,
‡
and
Srinivas Vemury
§
Department of Materials Science and Engineering, ML 0012, and Department of Chemical
Engineering, ML 0171, University of Cincinnati, Cincinnati, Ohio 45221, and Lucent
Technologies, G010, 2000 Northeast Expressway, Norcross, Georgia 30071
Received March 17, 1998. In Final Form: July 21, 1998
The morphology of flame-generated silica and titania aggregates is characterized by small-angle X-ray
scattering (SAXS). Nearly all these powders display mass-fractal morphologies, which are composed of
ramified aggregates of nanoscale primary particles. Primary particle size, aggregate size, fractal dimension,
and specific surface area are obtained from this analysis. The mass-fractal dimension varies from 2.5 to
1.6 for flame generated silica and titania aggregates in single and double diffusion flame reactors. However,
titania powders made in a single diffusion flame reactor appear as nonaggregates and nonfractals. Silica
powders synthesized with an imposed electric field in a laminar, premixed flame reactor are mass fractals
with narrowly confined fractal dimensions from 1.5 to 1.9 regardless of aggregate size.
Introduction
Aggregates of small primary particles can be produced
by various aerosol processes, including flame processes
for the production of materials such as titania, fumed silica,
and carbon black. During these processes, structural
features such as particle and aggregate size, structure,
and surface area vary, affecting the properties of the final
product.
1
Although aggregation behavior on molecular
or colloidal scales is important, relatively little attention
has been paid to it, partly because of the highly disordered
nature of these materials and difficulties in characteriza-
tion. However, with fractal concepts, the description of
morphological features of aggregates has been facilitated.
The primary tools for description of the morphology of
aggregates using fractals are electron microscopy
2-5
and
X-ray
6-9
or light scattering.
10,11
Megaridis and Dobbins
obtained a fractal dimension of about 1.7 for flame-
generated carbonaceous soot and fumed silica based on
transmission electron microscopy (TEM), suggesting that
cluster-cluster aggregation is an important growth
mechanism. More recently, Koylu et al.
3
analyzed flame
synthesized carbonaceous soot and found that aggregates
are mass-fractal with fractal dimension (d
f
) of about 1.7.
Although microscopy is quite useful in measurements of
primary particle size, it is generally difficult to obtain
primary particle size distribution from microscopy and
the measurement thus relies on a tedious process of
micrograph measurements. Microscopic characterization
of the morphology of secondary, mass-fractal structures
is even a more difficult and subjective process. Moreover,
the occlusion of 3-dimensional structure by overlap of a
number of aggregates or even superimposed structure from
the same aggregate, in a typical micrograph, makes the
process quite difficult.
Small-angle X-ray scattering (SAXS) offers an alternate
to this process since it is by nature a 3-dimensional
averaging technique with a direct measure of the radius
of gyration, R
g
. Characterization of 3-dimensional mass-
fractal morphologies is simple in a typical scattering
experiment. Combustion aerosol aggregates have been
characterized using SAXS in terms of a statistical
analysis.
6-9
Schaefer et al.
6
obtained fractal dimensions
between 1.7 and 1.9 for fumed silica aggregates from SAXS
and found that the surface of fumed silica is self-affine
with surface fractal dimensions between 2.5 and 3. For
these flame-generated silica powders, the features of
kinetic growth processes were also suggested. In addition
to SAXS, ultra small-angle X-ray scattering (USAXS)
scattering patterns can be extended to close to the
millimeter size scale by careful combination of SAXS data
with light scattering data. In the past, such combined
scattering curves and global scattering functions
12-14
have
been used to describe the three levels of structure for fine
powders, primary, secondary (aggregate) and tertiary
(agglomerate).
12-14
Fumed silica and titania powders made in a diffusion
flame reactor and a laminar, premixed flame reactor are
analyzed in this study. When particles are synthesized
in these reactors, the characteristics of the flame such as
mixing configuration or oxidant type can greatly affect
†
Department of Materials Science and Engineering, University
of Cincinnati.
‡
Department of Chemical Engineering, University of Cincinnati.
§
Lucent Technologies.
(1) Pratsinis, S. E. Prog. Energy Combust. 1998, 24 (3), 197.
(2) Megaridis, C. M.; Dobbins, R. A. Combust. Sci. Technol. 1995, 71,
95.
(3) Koylu, U. O.; Xing, Y.; Rosner, D. E. Langmuir 1995, 11, 4848.
(4) Neimark, A. V.; Koylu, L. O.; Rosner, D. E. J. Colloid Interface
Sci. 1996,180, 590.
(5) Samson, R. J.; Mulholland, G. W.; Gentry, J. W. Langmuir 1987,
3, 272.
(6) Schaefer, D. W.; Hurd, A. J. Aerosol Sci. Technol. 1990, 12, 876.
(7) Schaefer, D. W.; Keefer, K. D. In Fractals in Physics; Pietronero,
L., Tosatti, E., Eds.; Elsevier Science: Amsterdam, 1986; p 39.
(8) Schaefer, D. W. Mater. Res. Symp. Proc. 1987, 79, 47.
(9) Schaefer, D. W.; Martin, J. E.; Wiltzius, P.; Cannell, D. S. Phys.
Rev. Lett. 1984, 52, 2371.
(10) Oh, C.; Sorensen, C. M. J. Aerosol Sci. 1997, 28 (6), 937.
(11) Hurd, A. J.; Flower, W. L. J. Colloid Interface Sci. 1988, 122 (1),
178.
(12) Beaucage, G.; Schaefer, D. W. J. Non-Cryst. Solids 1994, 172-
174, 797.
(13) Beaucage, G. J. Appl. Cryst. 1995, 28, 717.
(14) Beaucage, G. J. Appl. Cryst. 1996, 29, 134.
5751 Langmuir 1998, 14, 5751-5756
S0743-7463(98)00308-4 CCC: $15.00 © 1998 American Chemical Society
Published on Web 08/26/1998