dispersion of spherical particles can vary from highly dispersed to totally aggregate
depending on the thermodynamics of the system and kinetics of samples preparation. The clustering of filler particles is favored by strong van der Waals forces.
–4
5
10
15
20
K (MPa)
–3
–2
–1
0
1
Log 10 t (s)
2
49 °C
26 °C
5 °C
Fig. 13 Relaxation function plotted against logarithmic time (log 10 t) for three different temperatures T ∈ {5, 26, 49}
o
C [77]
Fig. 14 Strain amplitude dependence of G* of N115 at different loadings (a) green compound, (b)
vulcanizate
210
G. Markovic ´ et al.
depending on the thermodynamics of the system and kinetics of samples preparation. The clustering of filler particles is favored by strong van der Waals forces.
–4
5
10
15
20
K (MPa)
–3
–2
–1
0
1
Log 10 t (s)
2
49 °C
26 °C
5 °C
Fig. 13 Relaxation function plotted against logarithmic time (log 10 t) for three different temperatures T ∈ {5, 26, 49}
o
C [77]
Fig. 14 Strain amplitude dependence of G* of N115 at different loadings (a) green compound, (b)
vulcanizate
210
G. Markovic ´ et al.