o_water_absorbtion.pdf
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Water Absorption
When an organic matrix composite is exposed to a humid environment or liquid, both the
moisture content and material temperature may change with time. These changes usually
degrade the mechanical properties of the laminate. The study of water absorption within
composites is based on the following parameters as a function of time: [4-26]
The temperature inside the material as a function of position;
The moisture concentration inside the material;
The total amount (mass) of moisture inside the material;
The moisture and temperature induced hygrothermal stress inside the
material;
The dimensional changes of the material; and
The mechanical, chemical, thermal or electric changes.
To determine the physical changes within a composite
laminate, the temperature distribution and moisture
content must be determined. When temperature varies
across the thickness only and equilibrium is quickly
achieved, the moisture and temperature distribution
process is called Fickian diffusion, which is
analogous to Fourier's equation for heat conduction.
Figure 4-13 illustrates some of the key parameters used
to describe the Fickian diffusion process in a
multilayered composite. The letter T refers to
temperature and the letter C refers to moistureconcentration.
Fick's second law of diffusion can be represented in
terms of three principal axes by the following
differential equation: [4-27]
=
+
+
c
tD
c
xD
c
xD
c
x
(4-7)
Figure 4-14 shows the change in moisture content, M, versus the square root of time. The
apparent plateau is characteristic of Fickian predictions, although experimental procedures haveshown behavior that varies from this. Additional water absorption has been attributed to the
relaxation of the polymer matrix under the influence of swelling stresses. [4-28] Figure 4-15
depicts some experimental results from investigations conducted at elevated temperatures.
Water Absorbtion Marine Composites
194
Figure 4-13 T i m e Va r y i n gEnvironmental Conditions in aM u lt i la y er e d C o mp o si t e[Springer, Environmental Ef-fects on Composite Materials]
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Structural designers are
primarily interested in
t h e l o n g t e r m
d e g r a d a t i o n o f
mechanical properties
w h en c o mp o si t es a r eimmersed in water. By
applying curve-fitting
p r o g r a m s t o
e x p e r i m e n t a l d a t a ,
extrapolations about long
term behavior can be
p o s t u l a t e d . [ 4 - 2 8 ]
Figure 4-16 depicts a 25
year prediction of shear
s t r e n g t h f o r g l a s s
p o l y es t e r s p e c im e n sdried after immersion.
S t r e n g t h v a l u e s
eventually level off at
a bo ut 6 0% o f t he ir
original value, with the
d e g r ad a t i on p r o c es s
accelerated at higher
temperatures. Figure
4-17 shows similar data
for wet tensile strength.
Experimental data at thehigher temperatures is in
relative agreement for
the first three years.
T ab le 4 -1 s ho ws t he
a p p a r e nt m a x i m um
moisture content and the
transverse diffusivities
for two polyester and
one vinyl ester E-glass
laminate. The numericaldesignation refers to
fiber content by weight.
The water content of laminates cannot be compared directly with cast resin water contents,
since the fibers generally do not absorb water. Water is concentrated in the resin
(approximately 75% by volume for bidirectional laminates and 67% by volume for
unidirectionals). [4-28]
195
Chapter Four PERFORMANCE
Figure 4-15 Time Varying Environmental Conditions in a Multi-layered Composite [Springer, Environmental Effects on Com-posite Materials]
Figure 4-14 Laminate Water Absorbtion Kinetics for Experi-mental Laminate Specimens [Pritchard, The Use of Water Ab-sorbtion Kinetic Data to Predict Laminate Property Changes]
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Table 4-1 Apparent Maximum Moisture Content and Transverse Diffusivities ofSome Polyester E-Glass and Vinyl Ester Laminates
[Springer, Environmental Effects on Composite Materials]
Substance Temp(C)
Maximum Moisture Content* Transverse Diffusivity
SMC-R25 VE SMC-R50 SMC-R50 SMC-R25 VE SMC-R50 SMC-R50
50% Humidity23 0.17 0.13 0.10 10.0 10.0 30.0
93 0.10 0.10 0.22 50.0 50.0 30.0
100%Humidity
23 1.00 0.63 1.35 10.0 5.0 9.0
93 0.30 0.40 0.56 50.0 50.0 50.0
Salt Water23 0.85 0.50 1.25 10.0 5.0 15.0
93 2.90 0.75 1.20 5.0 30.0 80.0
Diesel Fuel23 0.29 0.19 0.45 6.0 5.0 5.0
93 2.80 0.45 1.00 6.0 10.0 5.0
Lubricating Oil
23 0.25 0.20 0.30 10.0 10.0 10.0
93 0.60 0.10 0.25 10.0 10.0 10.0
Antifreeze23 0.45 0.30 0.65 50.0 30.0 20.0
93 4.25 3.50 2.25 5.0 0.8 10.0
*Values given in percent
Values given are D22x 10
7mm
2/sec
196
Water Absorbtion Marine Composites
Figure 4-16 Change of Moisture Con-tent with the Square Root of Time forFickian Diffusion [Springer, Environ-mental Effects on Composite Materials]
Figure 4-17 P r ed ic te d D ry S he arStrength versus Square Root of Immer-sion Time [Pritchard, The Use of WaterAbsorbtion Kinetic Data to Predict Lami-nate Property Changes]