CC BY
26
UDC 541.64
Yu. G. Yanovskii, G. V. Kozlov, G. E. Zaikov, Kh. S. Abzaldinov
THE STRUCTURE OF NANOFILLER IN ELASTOMERIC PARTICULATE-FILLED NANOCOMPOSITES
Keywords: Nanocomposite, nanofiller, structure, "chains", fractal analysis.
It has been shown that nanofiller particles (aggregates of particles) "chains" in elastomeric nanocomposites are physical fractal within the self-similarity (and, hence, fractality) range ~500-1450 nm. The low dimensions of nanofiller particles (aggregates of particles) structure in elastomeric nanocomposites are due to high fractal dimension of nanofiller initial particles surface.
Ключевые слова: нанокомпозит, нанонаполнитель, структура, "цепи ", фрактальный анализ.
Показано, что "цепи" частиц (агрегатов частиц) нанонаполнителя в эластомерных нанокомпозитах являются физическими фракталами в диапазоне самоподобия (и, следовательно, фрактальности) ~500-1450 нм. Небольшие размеры структуры частиц (агрегатов частиц) нанонаполнителя в эластомерных нанокомпозитах обусловлены большой фрактальной размерностью поверхности исходных частиц нанонаполнителя.
Introduction
It is well-known [1, 2], that in particulate-filled elastomeric nanocomposites (rubbers) nanofiller particles form linear spatial structures ("chains"). At the same time in polymer composites, filled with disperse microparticles (microcomposites) particles (aggregates of particles) of filler form a fractal network, which defines polymer matrix structure (analog of fractal lattice in computer simulation) [3, 4, 5]. This results to different mechanisms of polymer matrix structure formation in micro- and nanocomposites. If in the first filler particles (aggregates of particles) fractal network availability results to "disturbance" of polymer matrix structure, that is expressed in the increase of its fractal dimension df [3], then in case of polymer nanocomposites at nanofiller contents change the value df is not changed and equal to matrix polymer structure fractal dimension [6]. As it has to been expected, composites indicated classes structure formation mechanism change defines their properties change, in particular, reinforcement degree.
At present there are several methods of filler structure (distribution) determination in polymer matrix, both experimental [7, 8] and theoretical [3]. All the indicated methods describe this distribution by fractal dimension Dn of filler particles network. However, correct determination of any object fractal (Hausdorff) dimension includes three obligatory conditions. The first from them is the indicated above determination of fractal dimension numerical magnitude, which should not be equal to object topological dimension. As it is known [9], any real (physical) fractal possesses fractal properties within a certain scales range [10]. And at last, the third condition is the correct choice of measurement scales range itself. As it has been shown in papers [11, 12], the minimum range should exceed at any rate one self-similarity iteration.
The present paper purpose is dimension Dn estimation, both experimentally and theoretically, and checking two indicated above conditions fulfillment, i.e. obtaining of nanofiller particles (aggregates of particles) network ("chains") fractality strict proof in elastomeric
nanocomposites on the example of particulate-filled butadiene-styrene rubber.
Experimental
The elastomeric particulate-filled nanocomposite on the basis of butadiene-styrene rubber (BSR) was an object of the study. The technical carbon of mark № 220 (TC) of industrial production, nano- and microshungite (the mean filler particles size makes up 20, 40 and 200 nm, accordingly) were used as a filler. All fillers content makes up 37 mass %. Nano- and microdimensional disperse shungite particles were obtained from industrially extractive material by processing according to the original technology. A size and polydispersity of the received in milling process shungite particles were monitored with the aid of analytical disk centrifuge (CPS Instruments, Inc., USA), allowing to determine with high precision the size and distribution by sizes within the range from 2 nm up to 50 mcm.
Nanostructure was studied on atomic-power microscopes Nano-DST (Pacific Nanotechnology, USA) and Easy Scan DFM (Nanosurf, Switzerland) by semi-contact method in the force modulation regime. Atomic-power microscopy results were processed with the aid of specialized software package SPIP (Scanning Probe Image Processor, Denmark). SPIP is a powerful programmes package for processing of images, obtained on SPM, AFM, STM, scanning electron microscopes, transmission electron microscopes, interferometers, confocal microscopes, profilometers, optical microscopes and so on. The given package possesses the whole functions number, which are necessary at images precise analysis, in the number of which the following are included:
1) the possibility of three-dimensional reflecting objects obtaining, distortions automatized leveling, including Z-error mistakes removal for examination separate elements and so on;
2) quantitative analysis of particles or grains, more than 40 parameters can be calculated for each found particle or pore: area, perimeter, average diameter, the ratio of
linear sizes of grain width to its height distance between grains, coordinates of grain center of mass a.a. can be presented in a diagram form or in a histogram form.
Results and Discussion
The first method of dimension Dn experimental determination uses the following fractal relationship [13, 14]: D ln N
Dn --(1)
ln p
where N is a number of particles with size p.
Particles sizes were established on the basis of atomic-power microscopy data (see Fig. 1). For each from the three studied nanocomposites no less than 200 particles were measured, the sizes of which were united into 10 groups and mean values N and p were obtained.
r w V** in }t 44 '»Sr. i««&m»»n w
* j
\ tk .
JL '
' m. - - 4. ...
.¿A ' y 1
tA I
the values Dn were calculated according to their slope (see Fig. 2). It is obvious, that at such approach fractal dimension Dn is determined in two-dimensional Euclidean space, whereas real nanocomposite should be considered in three-dimensional Euclidean space. The following relationship can be used for Dn re-calculation for the case of three-dimensional space [15]:
,_ d + D2 ±[(d - D2)2 - 2}/2
'_ 2 where D3 and D2 are corresponding fractal dimensions in three- and two-dimensional Euclidean spaces, d=3.
ln N
D3 _-
(2)
0
3.0
ln p
Fig. 2 - The dependence of nanofiller particles number N on their size p for nanocomposites BSR/TC (1), BSR/nanoshungite (2) and BSR/microshungite (3)
The calculated according to the indicated method dimensions Dn are adduced in table 1. As it follows from the data of this table, the values Dn for the studied nanocomposites are varied within the range of 1.10-1.36, i.e. they characterize more or less branched linear formations ("chains") of nanofiller particles (aggregates of particles) in elastomeric nanocomposite structure.
Table 1 - The dimensions of nanofiller particles (aggregates of particles) structure in elastomeric
The nano D„, D„, d0 dsurf Dn,
composite the the the
equa equat equa
tions ions tions
(1) (3) (7)
BSR/TC 1.19 1.17 2.86 2.64 0.48 1.11
BSR/nano 1.10 1.10 2.81 2.56 0.36 0.78
shungite
BSR/micro 1.36 1.39 2.41 2.39 0.32 1.47
shungite
4
2
a
b
c
Fig. 1 - The electron micrographs of nanocomposites BSR/TC (a), BSR/nanoshungite (b) and BSR/microshungite (c), obtained by atomic-power microscopy in the force modulation regime
The dependences N(p) in double logarithmic coordinates were plotted, which proved to be linear and
Let us remind that for particulate-filled composites polyhydroxiether/graphite the value Dn changes within the range of ~ 2.30-2.80 [7], i.e. for these materials filler particles network is a bulk object, but not a linear one [9].
Another method of Dn experimental determination uses the so-called "quadrates method" [16]. Its essence consists in the following. On the enlarged nanocomposite microphotograph (see Fig. 1) a
net of quadrates with quadrate side size a,-, changing from 4.5 up to 24 mm with constant ratio a,+i/a,=1.5, is applied and then quadrates number N,, in to which nanofiller particles hit (fully or partly), is calculated. Five arbitrary net positions concerning microphotograph were chosen for each measurement. If nanofiller particles network is fractal, then the following relationship should be fulfilled [16]:
Ni-N,
n, ~ s:
(3)
where Si is quadrate area, which is equal to .
In Fig. 3 the dependences of N on St in double logarithmic coordinates for the three studied nanocomposites, corresponding to the relationship (3), is adduced.
30
20
10
10
15
s: D-/2 xi0-3
ln N,
6
ln S,
Fig. 3 - The dependences of covering quadrates number Ni on their area Si, corresponding to the relationship (3), in double logarithmic coordinates for nanocomposites on the basis of BSR. The designations are the same, that in Fig. 2
As one can see, these dependences are linear, that allows to determine the value Dn from their slope. The determined according to the relationship (3) values Dn are also adduced in table 1, from which a good correspondence of dimensions Dn, obtained by the two described above methods, follows (their average discrepancy makes up 2.1 % after these dimensions recalculation for three dimensional space according to the equation (2)).
As it has been shown in paper [17], at the relationship (3) the usage for self-similar fractal objects the condition should be fulfilled:
N : N,:1~
s:
(4)
In Fig. 4 the dependence, corresponding to the relationship (4), for the three studied elastomeric nanocomposites is adduced. As one can see, this dependence is linear, passes through coordinates origin, that according to the relationship (4) is confirmed by nanofiller particles (aggregates of particles) "chains" self-similarity within the selected a,- range. It is obvious, that this self-similarity will be a statistical one [17].
Fig. 4 - The dependences of (Ni-Ni+1) on the value
S-Dn 2, corresponding to the relationship (4), for
nanocomposites on the basis of BSR. The designations are the same, that in Fig. 2
Let us note, that the points, corresponding to a,= 16 mm for nanocomposites BSR/TC and BSR/microshungite, do not correspond to a common straight line. Accounting for electron microphotographs of Fig. 1 enlargement this gives the self-similarity range for nanofiller "chains" of 464-1472 nm. For nanocomposite BSR/nanoshungite, which has no points deviating from a straight line of Fig. 4, a, range makes up 311-1510 nm, that corresponds well enough to the indicated above self-similarity range.
In papers [11, 12] it has been shown, that measurement scales S, minimum range should contained at least one self-similarity iteration. In this case the condition for ratio of maximum Smax and minimum Smin areas of covering quadrates should be fulfilled [12]:
Sm
Sm
■ > 22/D-
(5)
Hence, accounting for the defined above restriction let us obtain Smax/Smin=121/20.25=5.975, that
is larger than values 22 Dn for the studied nanocomposites, which are equal to 2.71-3.52. This means, that measurement scales range is chosen correctly.
The self-similarity iterations number ц can be estimated from the inequality [12]:
(
Sm
Y
s
V mm У
> 2м
(6)
Using the indicated above values of the included in the inequality (6) parameters, ц=1.42-1.75 is obtained for the studied nanocomposites, i.e. in our experiment conditions self-similarity iterations number is larger than unity, that again is confirmed by the value Dn estimation correctness [8].
And let us consider in conclusion the physical grounds of smaller values Dn for elastomeric nanocomposites in comparison with polymer microcomposites, i.e. the causes of nanofiller particles
0
5
4
2
4
6
D
n
(aggregates of particles) "chains" formation in the first. The value Dn can be determined theoretically according to the equation [3]:
4V
Dn + 2.55d0 - 7.10 4.18
(7)
where ф^ is interfacial regions relative fraction, d0 is nanofiller initial particles surface dimension.
The dimension d0 estimation can be carried out with the aid of the relationship [6]:
/D \do-d
S = 410
2
(8)
where Su is nanofiller initial particles specific surface in m2/g, Dp is their diameter in nm, d is dimension of Euclidean space, in which a fractal is considered (it is obvious, in our case d=3).
The value Su can be calculated according to the equation [18]:
S 6
Su = 7D (9)
PnDp
where pn is nanofiller density, which is determined according to the empirical formula [6]:
Pn = 0.188(Dp )/3 (10)
The results of value d0 theoretical estimation are adduced in table 1. The value ф,у can be calculated according to the equation [6]:
фг/ =Фп (dsurf " 2) (11)
where фп is nanofiller volume fraction, dsurf is fractal dimension of nanoparticles aggregate surface.
The value фп is determined according to the equation [6]:
фп = — (12)
Pn
where Wn is nanofiller mass fraction and dimension dsurf is calculated according to the equations (8)-(10) at diameter Dp replacement on nanoparticles aggregate diameter Dagr, which is determined experimentally (see Fig. 5).
600,0-f'' 500,0"'' 400,0-'' x 300,0- ^ 200,0-^ 100,0-И 0,0
□ a
□ b □ c
technical carbon nanoshungite microshungite
Fig. 5 - The initial particles diameter (a), their aggregates size in nanocomposite (b) and distance between nanoparticles aggregates (c) for nanocomposites on the basis of BSR, filled with technical carbon, nano- and microshungite
The results of dimension Dn theoretical calculation according to the equations (7)-(12) are
adduced in table 1, from which theory and experiment good correspondence follows. The equation (7) indicates unequivocally the cause of filler in nano- and microcomposites different behaviour. The high (close to 3, see table 1) values d0 for nanoparticles and relatively small (d0=2.17 for graphite) values d0 for microparticles at comparable values ф^ for composites of the indicated classes [3, 6].
Conclusions
Therefore, the present paper results have shown, that nanofiller particles (aggregates of particles) "chains" in elastomeric nanocomposites are physical fractal within self-similarity (and, hence, fractality [14]) range of ~ 500-1450 nm. In this range their dimension Dn can be estimated according to the equations (1), (3) and (7). The cited examples demonstrate the necessity of the measurement scales range correct choice. As it has been noted earlier [19], linearity of the plots, corresponding to the equations (1) and (3), and Dn nonintegral value do not guarantee object self-similarity (and, hence, fractality). The nanofiller particles (aggregates of particles) structure low dimensions are due to the initial nanofiller particles surface high fractal dimension.
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© Yu. G. Yanovskii - professor, director of Russian Academy of Sciences Institute of Applied Mechanics; G. V. Kozlov - senior researcher of FSBEI HPE "Kh.M. Berbekov Kabardino-Balkarian State University"; G. E. Zaikov - professor of Kazan National Research Technological University; Kh. S. Abzaldinov - docent of Kazan National Research Technological University, ov_stoyanov@mail.ru.
