Chemistry Reference
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of the material, and the average molecular weight between cross-links. In terms
of nominal strain this equation is approximately
2
τ 5 ðρ
RT
=
M c Þð
3
ε1
3
ε
1 ...
(4-30)
and at low strains, Young's modulus, Y ,is
Y
d
τ=
d
ε5
3
ρ
RT
=
M c
(4-31)
The more tightly cross-linked the elastomer, the lower will be M c and the
higher will be its modulus. That is, it will take more force to extend the polymer
a given amount at fixed temperature. Also, because the elastomer is an entropy
spring, the modulus will increase with temperature.
Equation (4-29) is valid for small extensions only. The actual behavior of real
cross-linked elastomers in uniaxial extension is described by the Mooney
Rivlin
equation which is similar in form to Eq. (4-29) :
2
τ 5 ð
C 1 1
C 2 =ΛÞðΛ2
1
Þ
(4-32)
Here C 1 and C 2 are empirical constants, and C 1 is often assumed to be equal
to
ρ
RT/M c .
EXAMPLE 4-1
Given an SBR rubber (23.5 mol% styrene) that has an
M n of 100,000 before cross-linking.
/m 2 at 100% elongation of the cross-
Calculate the engineering stress in the units of
MN
linked elastomer with an
M c of 10,000 at 25 C. Also calculate the corresponding modulus
at very low extensions. The density of the cross-linked elastomer is 0.98 g/cm 3 .
A 100% elongation means that
Λ5
2
λ 0 /
λ5
2.
τ
and
Y
can be calculated using Eqs. (4-
29) and (4-31) , respectively.
5
0:98310 6
38:31433298
10;000
1
4
000 m 2 5
425 M m 2
τ 5
2
2
425
;
0
:
330:98310 6
38:31433298
10;000
000 m 2 5
728 M m 2
Y 5
5
728
;
0
:
4.5.2.4 Real and Ideal Rubbers
To this point, we have emphasized that the retractive force in a stretched ideal
elastomer is directly proportional to its temperature. In a cross-linked, real elasto-
mer that has been reinforced with carbon black, as is the usual practice, the force
to produce a given elongation may actually be seen to decrease with increased
temperature. This is because the anchor regions that hold the elastomer chains
together are not only chemical cross-links, as assumed in the ideal theory. They
also comprise physical entanglements of polymer molecules and rubber-carbon
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