In order to establish the relationship between the distribution function
Fτ(τ) of relaxation time τ and the shape and the characteristic parameters of dynamic loss tangent (tanΔ)-temperature (
T) curves, theoretical equations representing tanΔ-
T curves are derived; seven functions given by
Fτ(τ)=
kn'τ
n' and three functions given by triangles. WLF and Arrhenius types are assumed for temperature dependence of τ. On the basis of these theoretical equations, tanΔ-
T curves are numerically calculated. In the case of
n'_??_0, the peak value of tanΔ-
T curve, (tanΔ)
max, peak temperature
Tmax and the ratio of half value width Δ
T1/2/Δ
T1/2 (s) (the suffix
s indicates the system composing of a single relaxation time) depend on those factors as the average relaxation time τ,
Fτ, the total number of Maxwell elements in a system
N, the ratio of elastic modulus before and after relaxation α, and the minimum relaxation time τ
l in
Fτ(τ). In the case of
n'_??_-0.5, a significant shoulder is observed on tanΔ-
T curves in the lower temperature region than
Tmax. The necessary condition to have this shoulder is (tanΔ)
max_??_3.5/(
n'+3)
4 and
N_??_√<10>, The tanΔ-
T curve (especially, Δ
T1/2/Δ
T1/2 (s) ), measured in the temperature range in which appears the dynamic absorption arising from microbrownian movement of polymer segments in amorphous region of semi-crystalline polymers (α
a), is remarkably different from that calculated by using the above mentioned functions for
Fτ(τ). Contrary to this, tanΔ-
T curves determined experimentally in the temperature range of α
a absorption of amorphous polymers are in good agreement with those calculated by using
n'=-2-0. In the actual experiment, no shoulder, is observed on tanΔ-
T curves for both amorphous and semi-crystalline polymers.
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