Solution to Problems of Chapter 4
4.1 Suppose that the relaxation function for a linear viscoelastic material is given
by
!
G(t) =100(1+9et 2 )
lb/in2 .
(a) Starting with the integral relation (4.1) or (4.2) between G(t) and J(t), and using the
Laplace transform, derive the corresponding form for J(t).
(b) Verify that J(0) = 1/G(0) and J() = 1/G( ).
(c) Calculate
!
R
and
!
C
using Definition 1 for the creep and relaxation times.
Are they related by (4.24)?
(d) Show that
!
G(t)J(t) 1
by means of a plot.
SOLUTION
(a) The integral relation between the creep and stress relaxation functions is
1=G(0)J(t) +J(t s) ˙
G (s)ds
0
t
#
Apply the Laplace transform
!
a2100
a a +12
( )
=
a+1
2
( )
!
(b)
G(0) =100 10 G(#)=100
J(0) =1
100 19
10
#
$
% &
( =1
1000 J())=1
100
!
!
!
!
!
R=#1000 #100
$
=2
!
C=
1
100 #1
1000
9
$
=20
!
!
C
and
!
R
are related by (4.24)
(d)
4.2 Consider the creep function
!
J(t) =1
1000 10 5et 4 3et 8
[ ]
.
(a) Sketch a graph of
!
J(t)
, and label significant values.
(b) Show that the corresponding stress relaxation function also is the sum of a constant
and two exponentials, i.e. it has the form
!
G(t) =Co+C1et#1+C2et#2
,
where
!
Co, C1, C2
and
!
1,2
are constants. It is not necessary to find them.
(c) Calculate the characteristic creep time
!
C
, as given by Definition 1. What is the
corresponding value of the characteristic stress relaxation time
!
R
(d) Calculate the value of
!
Co
and of the sum
!
C1+C2
.
SOLUTION
(a)
(b) The integral relation between the creep and stress relaxation functions is
!
1=G(0)J(t) +J(t s) ˙
G (s)ds
0
t
#
Applying the Laplace transform
!
G (a) =1
a2J (a)
The Laplace transform of J(t) is
!
J (a) =1
1000
10
a51
a+14
31
a+18
#
$
%
%
&
(
(
=1
1000
10 a +1
4
( )
a+1
8
( )
5a a +1
8
( )
3a a +1
4
( )
!
G(t) =Co+C1et#1+C2et#2
(c)
!
C=J(#)$J(0)
˙
J (0)
!
J(0) =2
1000 J()=10
1000
˙
J (t) =1
1000
5
4et 4 +3
8et 8
#
$
%
&
( ˙
J (0) =13
8
1
1000
!
1000
8
!
R=G(#)
G(0) C=J(0)
J(#)C=128
130 =0.984
(d)
!
Co=G()=1
J()=1000
10 =100
!
!
C1+C2=1
J(0) Co=1000
21000
10 =400