An anisotropic rotary diffusion model for fiber orientation in short- and long-fiber thermoplastics

Abstract The Folgar–Tucker model, which is widely-used to predict fiber orientation in injection-molded composites, accounts for fiber–fiber interactions using isotropic rotary diffusion. However, this model does not match all aspects of experimental fiber orientation data, especially for composites with long discontinuous fibers. This paper develops a fiber orientation model that incorporates anisotropic rotary diffusion. From kinetic theory we derive the evolution equation for the second-order orientation tensor, correcting some errors in earlier treatments. The diffusivity is assumed to depend on a second-order space tensor, which is taken to be a function of the orientation state and the rate of deformation. Model parameters are selected by matching the experimental steady-state orientation in simple shear flow, and by requiring stable steady states and physically realizable solutions. Also, concentrated fiber suspensions align more slowly with respect to strain than models based on Jeffery's equation, and we incorporate this behavior in an objective way. The final model is suitable for use in mold filling and other flow simulations, and it gives improved predictions of fiber orientation for injection molded long-fiber composites.

[1]  Nhan Phan-Thien,et al.  A direct simulation of fibre suspensions , 1998 .

[2]  C. L. Tucker,et al.  Orientation Behavior of Fibers in Concentrated Suspensions , 1984 .

[3]  Charles L. Tucker,et al.  Orthotropic closure approximations for flow-induced fiber orientation , 1995 .

[4]  George L. Hand,et al.  A theory of anisotropic fluids , 1962, Journal of Fluid Mechanics.

[5]  D. E. Smith,et al.  An invariant based fitted closure of the sixth-order orientation tensor for modeling short-fiber suspensions , 2005 .

[6]  Charles L. Tucker,et al.  Fiber orientation in simple injection moldings. Part I: Theory and numerical methods , 1991 .

[7]  N. Phan-Thien,et al.  Folgar–Tucker constant for a fibre suspension in a Newtonian fluid , 2002 .

[8]  Charles L. Tucker,et al.  Fiber orientation in simple injection moldings. Part II: Experimental results , 1992 .

[9]  Charles L. Tucker,et al.  An objective model for slow orientation kinetics in concentrated fiber suspensions: Theory and rheological evidence , 2008 .

[10]  S. F. Shen,et al.  A finite-element/finite-difference simulation of the injection-molding filling process , 1980 .

[11]  Suresh G. Advani,et al.  Fiber–fiber interactions in homogeneous flows of nondilute suspensions , 1991 .

[12]  Peter Hine,et al.  Hydrostatically extruded glass‐fiber‐reinforced polyoxymethylene. I: The development of fiber and matrix orientation , 1996 .

[13]  G. B. Jeffery The motion of ellipsoidal particles immersed in a viscous fluid , 1922 .

[14]  Suresh G. Advani,et al.  The Use of Tensors to Describe and Predict Fiber Orientation in Short Fiber Composites , 1987 .

[15]  R. Aris Vectors, Tensors and the Basic Equations of Fluid Mechanics , 1962 .

[16]  D. Koch A model for orientational diffusion in fiber suspensions , 1995 .

[17]  Jin Wang,et al.  Improved fiber orientation predictions for injection molded composites , 2007 .

[18]  Ba Nghiep Nguyen,et al.  Fiber Length and Orientation in Long-Fiber Injection-Molded Thermoplastics — Part I: Modeling of Microstructure and Elastic Properties , 2008 .

[19]  P. Carreau,et al.  Rheological properties of short fiber filled polypropylene in transient shear flow , 2004 .