In rubber-blended polymer, the onset of cavitation in the particles relaxes the high triaxiality stress state and suppresses the onset of crazing in the polymer. As a result, large plastic deformation is substantially promoted compared with single-phase polymer. On the other hand, it is also well known that the onset of cavitation depends on the size of particle. To investigate the size dependence of cavitation behavior in the particle, a theoretical analysis is done employing a void model under plane strain condition, which takes into account the surface tension and the limiting stretch of the void. Continuously, to study the effect of the size-dependent cavitation on the micro- to macroscopic mechanical behavior of the blend, a computational model is proposed for the blend consisting of irregularly distributed heterogeneous particles containing the void with surface force. The results indicate that when the size of the particle decreases to a critical value that depends on both the initial shear modulus of particle and the surface tension on the surface of void, the increase of the critical stress for the onset of cavitation becomes remarkable and consequently, the onset of cavitation is eliminated. When the particle is embedded in polymer, the relation between average normal stress, which is acting on the interface of particle and matrix, and volumetric strain of particle shows dependence on the size of particle but no dependence on the triaxiality of macroscopic loading condition. For the blend consisting of particles smaller than the critical value, the onset of cavitation is eliminated in particles and as a result, the conformation of the shape of particle to the localized shear band in matrix becomes difficult and the shear deformation behavior tends to occur all over the matrix. Furthermore, in this case, the area of the maximum mean stress is confined to the area adjacent to the particle and the value of it increases almost linearly throughout the whole deformation process, which would lead to the onset of crazing in matrix. On the other hand, it is clarified that the onset of cavitation is predominant in the localized microscopic region containing heterogeneous particles and therefore, the plastic deformation is promoted in this region.

1.
Bucknall
,
C. B.
, 1977,
Toughened Plastics
,
Applied Science
,
Barking, Essex, England
, Chap. 7.
2.
Gent
,
A. N.
, and
Lindley
,
P. B.
, 1958, “
Internal Rupture of Bonded Rubber Cylinders in Tension
,”
Proc. R. Soc. London, Ser. A
1364-5021,
249
, pp.
195
204
.
3.
Ball
,
J. M.
, 1982, “
Discontinuous Equilibrium Solutions and Cavitation in Nonlinear Elasticity
,”
Philos. Trans. R. Soc. London, Ser. A
0962-8428,
306
, pp.
557
611
.
4.
Horgan
,
C. O.
, and
Abeyarantne
,
R.
, 1986, “
A Bifurcation Problem for a Compressible Nonlinearly Elastic Medium: Growth of a Microvoid
,”
J. Elast.
0374-3535,
16
, pp.
189
200
.
5.
Hou
,
H.
, and
Abeyaratne
,
R.
, 1992, “
Cavitation in Elastic and Elastic-Plastic Solids
,”
J. Mech. Phys. Solids
0022-5096,
40
, pp.
571
592
.
6.
Gent
,
A. N.
, and
Tompkins
,
D. A.
, 1969, “
Surface Energy Effects for Small Holes or Particles in Elastomers
,”
J. Polym. Sci., Part A-2
0098-1273,
7
, pp.
1483
1488
.
7.
Lazzeri
,
A.
, and
Bucknall
,
C. B.
, 1995, “
Applications of a Dilatational Yielding Model to Rubber-Toughened Polymers
,”
Polymer
0032-3861,
36
, pp.
2895
2902
.
8.
Fond
,
C.
,
Lobbrecht
,
A.
, and
Schirrer
,
R.
, 1996, “
Polymers Toughened With Rubber Microspheres: An Analytical Solution for Stresses and Strains in the Rubber Particles at Equilibrium and Rupture
,”
Int. J. Fract.
0376-9429,
77
, pp.
141
159
.
9.
Williams
,
M. L.
, and
Schapery
,
R. A.
, 1965, “
Spherical Flaw Instability in Hydrostatic Tension
,”
Int. J. Fract. Mech.
0020-7268,
1
, pp.
64
71
.
10.
Gent
,
A. N.
, and
Wang
,
C.
, 1991, “
Fracture Mechanics and Cavitation in Rubber-Like Solids
,”
J. Mater. Sci.
0022-2461,
26
, pp.
3392
3395
.
11.
Diani
,
J.
, 2001, “
Irreversible Growth of a Spherical Cavity in Rubber-Like Material: A Fracture Mechanics Description
,”
Int. J. Fract.
0376-9429,
112
, pp.
151
161
.
12.
Haward
,
R. N.
, and
Owen
,
D. R. J.
, 1973, “
The Yielding of a Two-Dimensional Void Assembly in an Organic Glass
,”
J. Mater. Sci.
0022-2461,
8
, pp.
1136
1144
.
13.
Sue
,
H. J.
, and
Yee
,
A. F.
, 1988, “
Deformation Behavior of a Polycarbonate Plate With a Circular Hole: Finite Element Model and Experimental Observations
,”
Polymer
0032-3861,
29
, pp.
1619
1624
.
14.
Steenbrink
,
A. C.
,
Van der Giessen
,
E.
, and
Wu
,
P. D.
, 1997, “
Void Growth in Glassy Polymers
,”
J. Mech. Phys. Solids
0022-5096,
45
, pp.
405
437
.
15.
Tomita
,
Y.
, and
Lu
,
W.
, 2002, “
Characterization of Micro- to Macroscopic Response of Polymers Containing Voids Under Macroscopically Uniform Deformation
,”
Int. J. Solids Struct.
0020-7683,
39
, pp.
3409
3428
.
16.
Smit
,
R. J. M.
,
Brekelmans
,
W. A. M.
, and
Meijer
,
H. E. H.
, 1999, “
Prediction of the Larger-Strain Mechanical Response of Heterogeneous Polymer Systems: Local and Global Deformation Behavior of a Representative Volume Element of Voided Polycarbonate
,”
J. Mech. Phys. Solids
0022-5096,
47
, pp.
201
221
.
17.
Steenbrink
,
A. C.
, and
Van der Giessen
,
E.
, 1999, “
On Cavitation, Post-Cavitation and Yield in Amorphous Polymer-Rubber Blends
,”
J. Mech. Phys. Solids
0022-5096,
47
, pp.
843
876
.
18.
Tomita
,
Y.
, and
Lu
,
W.
, 2002, “
Computational Characterization of Micro- to Macroscopic Mechanical Behavior and Damage of Polymers Containing Second-Phase Particles
,”
Int. J. Form. Processes
1292-7775,
5
, pp.
521
530
.
19.
Arruda
,
E. M.
, and
Boyce
,
M. C.
, 1993, “
A Three-Dimensional Constitutive Model for the Large Stretch Behavior of Rubber Elastic Materials
,”
J. Mech. Phys. Solids
0022-5096,
41
, pp.
389
412
.
20.
Tomita
,
Y.
,
Adachi
,
T.
, and
Tanaka
,
S.
, 1997, “
Modeling and Application of Constitutive Equation for Glassy Polymer Based on Nonaffine Network Theory
,”
Eur. J. Mech. A/Solids
0997-7538,
16
, pp.
745
755
.
21.
Argon
,
A. S.
, 1973, “
A Theory for the Low-Temperature Plastic Deformation of Glassy Polymers
,”
Philos. Mag.
0031-8086,
28
, pp.
839
865
.
22.
Boyce
,
M. C.
,
Park
,
D. M.
, and
Argon
,
A. S.
, 1988, “
Large Inelastic Deformation of Glassy Polymers. Part 1: Rate Dependent Constitutive Model
,”
Mech. Mater.
0167-6636,
7
, pp.
15
33
.
23.
Higa
,
Y.
, and
Tomita
,
Y.
, 1999, “
Computational Prediction of Mechanical Properties of Nickel-Based Superalloy with Gamma Prime Phase Precipitates
,”
Proceedings of ICM8
(Victoria, B.C., Canada), Vol.
III
, pp.
1095
1099
.
24.
Fond
,
C.
, 2001, “
Cavitation Criterion for Rubber Materials: A Review of Void Growth Models
,”
J. Polym. Sci., Part B: Polym. Phys.
0887-6266,
39
, pp.
2081
2096
.
25.
Pearson
,
R. A.
, and
Yee
,
A. F.
, 1986, “
Toughening Mechanisms in Elastomer-Modified Epoxies
,”
J. Mater. Sci.
0022-2461,
21
, pp.
2475
2488
.
26.
Sternstein
,
S. S.
, and
Ongchin
,
L.
, 1969, “
Yield Criteria for Plastic Deformation of Glassy High Polymers in General Stress Fields
,”
Polym. Prepr. (Am. Chem. Soc. Div. Polym. Chem.)
0032-3934,
10
, pp.
1117
1124
.
27.
Griffith
,
A. A.
, 1921, “
The Phenomena of Rupture and Flow in Solids
,”
Philos. Trans. R. Soc. London, Ser. A
0962-8428,
331
, pp.
163
198
.
You do not currently have access to this content.