Fig. 11 Linear elastic and viscous modulus functions G
0 (ω, T ) and G
00 (ω, T ) of a SBR1500/50phr
N330 carbon black compound, drawn using the λ i , G i of a six elements generalized Maxwell model
and the respective C1, C2 parameters of a WLF-type equation with 100
C as reference temperature; experimental data from a frequency-temperature sweep protocol at 1 deg. strain amplitude
with a closed-cavity torsional harmonic rheometer are plotted in comparison with calculated maps
Fig. 12 Dynamic Viscosity function of gum EPDM2504 at 100
C; author’s experimental data
and fitted Carreau-Yasuda model
290
J.L. Leblanc
0 (ω, T ) and G
00 (ω, T ) of a SBR1500/50phr
N330 carbon black compound, drawn using the λ i , G i of a six elements generalized Maxwell model
and the respective C1, C2 parameters of a WLF-type equation with 100
C as reference temperature; experimental data from a frequency-temperature sweep protocol at 1 deg. strain amplitude
with a closed-cavity torsional harmonic rheometer are plotted in comparison with calculated maps
Fig. 12 Dynamic Viscosity function of gum EPDM2504 at 100
C; author’s experimental data
and fitted Carreau-Yasuda model
290
J.L. Leblanc