Advances in Mathematical Physics

Volume 2017, Article ID 4780928, 11 pages

https://doi.org/10.1155/2017/4780928

## Contrast Expansion Method for Elastic Incompressible Fibrous Composites

^{1}Department of Differential Equations and Statistics, Faculty of Mathematics and Natural Sciences, University of Rzeszow, Pigonia 1, 35-959 Rzeszow, Poland^{2}Pedagogical University, Ul. Podchorazych 2, 30-084 Krakow, Poland

Correspondence should be addressed to Vladimir Mityushev; lp.wokark.pu@uytim

Received 31 May 2017; Accepted 14 September 2017; Published 17 October 2017

Academic Editor: Andrei D. Mironov

Copyright © 2017 Piotr Drygaś and Vladimir Mityushev. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

Contrast parameter expansion of the elastic fields for 2D composites is developed by Schwarz’s method and by the method of functional equations for the case of circular inclusions. A computationally efficient algorithm is described and implemented in symbolic form to compute the local fields in 2D elastic composites and the effective shear modulus for macroscopically isotropic composites. The obtained new analytical formula contains high-order terms in the contrast parameter and explicitly demonstrates dependence on the location of inclusions. As a numerical example, the hexagonal array is considered.

#### 1. Introduction

The general potential theory of mathematical physics yields methods of integral equation to numerically solve various boundary value problems. Integral equations for plane elastic problems were constructed by Muskhelishvili [1], first, extended to doubly periodic problems in [2], and developed in [3–5] and papers cited therein. The obtained results were applied to computations of the effective properties of the elastic media. Integral equations are efficient for the numerical investigation of nondilute composites when interactions of inclusions have to be taken into account. Another type of integral equation based on the generalized alternating method of Schwarz was proposed by Mikhlin [6] and developed in [7].

Consider a problem on the plane isomorphic to the complex plane . Let where the boundary of is a simple closed Lyapunov curve oriented in clockwise sense. Schwarz’s method for a multiply-connected domain is based on the separate solutions of the simple boundary value problems for simply connected domains . It was demonstrated in [7] that Schwarz’s method can be realized as the iterative schemes constructed on contrast and on concentration parameters considered as small perturbation parameters and precisely described below. Convergence was proved for Laplace’s equation for the contrast expansion.

The main advantage of Schwarz’s method consists in analytical solution to the problems discussed when the physical parameters are presented in symbolic form in the final exact or approximate formulae. Such formulae were recently obtained in [8] for biharmonic functions which describes elastic materials for a circular multiply-connected domain. The results of [8] are based on the concentration expansion.

In the present paper, we apply Schwarz’s method based on the contrast parameter expansion for a circular multiply-connected domain. Schwarz’s method is used in the form of the functional equations method [7–9]. Elastic isotropic materials are described through two independent moduli. In order to make the presentation clear, we simplify the problem by consideration of incompressible materials when Poisson’s ratio is equal to . Then, we introduce only one contrast parameter:where and denote the shear modulus of inclusions and matrix , respectively.

In the present paper, we deduce a computationally efficient algorithm implemented in symbolic form to compute the local fields in 2D elastic composites and the effective shear modulus for macroscopically isotropic composites. The obtained new analytical formula is valid up to and explicitly demonstrates dependence on the location of inclusions. Such an approach has advantages over pure numerical methods when dependencies of the effective constants on the mechanical properties of constitutes and on geometrical structure are required.

The numerical examples from Section 6 give sufficiently accurate values of for all admissible , that is, for and for not exceeding .

#### 2. Contrast Expansion Method

Consider a finite number of inclusions as mutually disjoint simply connected domains in the complex plane . It is worth noting that the number is given in a symbolic form with an implicit purpose to pass to the limit later.

The components of the stress tensor can be determined by the Kolosov-Muskhelishvili formulae [1]: The strain tensor components of incompressible materials , are determined by the formulae [1]: Let the stress tensor be applied at infinity:The uniform shear stress will be considered in the paper when Then, where the functions and are analytical in and bounded at infinity. The functions and are analytical in and twice differentiable in the closures of the considered domains.

It follows from (1) that The perfect bonding at the matrix-inclusion interface can be expressed by two equations [1]: The problem (8)-(9) is the classic boundary value problem of the plane elasticity having the unique solution up to additive constants corresponding to rigid shifts of medium. It follows from [1] that solutions of (8)-(9) analytically depend on for sufficiently small . One can see also Chapter 2, Section in [3], where the problem (8)-(9) is reduced to the Fredholm integral equation shortly written as where is a compact integral operator in the space of the Hölder continuous functions.

We are looking for the complex potentials in the contrast expansion form. For instance, for sufficiently small has the following form: Then, the problem (8)-(9) is reduced to the following cascade of boundary value problems. Equation (8) becomesEquation (9) yields the cascade where

Addition and subtraction of the boundary condition (12) for and the first condition (13) yield Application of principle of analytic continuation to (15) implies analytic continuation of the functions and into all the domains . Then, (6) gives the exact formulae for the zero approximation: and .

Ultimately, we arrive at the following cascade. First, we solve boundary value problems separately for every domain : Next, we solve the problem following from (13): This is a boundary value problem for the multiply-connected domain on the functions , analytic in and twice continuously differentiable in the closure of including infinity. The described above step is the first step of the iterative scheme when we pass from and to and . The step consists in the solution to the problems for every domain : and, further, the problem for the domain

Therefore, the conjugation problem (8)-(9) is reduced to the sequence of the problems separately for the domains () and . The described iterative scheme is computationally effective if the inclusions have simple shape. The next section is devoted to its explicit realization for circular inclusions.

#### 3. Method of Functional Equations

Consider the circular inclusions and , where . Introduce the new unknown functions analytic in except at the point , where its principal part has the form

Let denote the inversion with respect to the circle . If a function is analytic in , then is analytic in The problem (8), (9) was reduced in [9] (see equations (5.6.11) and (5.6.16) in Chapter 5), [10] to the system of functional equations: where and are constants. The unknown functions and () are related by equations (22)-(23). One can see that the functional equations do not contain integral operators but contain compositions of and with inversions.

Following [11], we first introduce the Hardy-Sobolev space separately for each as the space of functions analytic in satisfying the conditions: where denotes the derivative . The norm is introduced as follows:where the classic Hardy norm is used.

Using the above designations (24)–(26) we introduce the space shortly denoted by of functions analytic in endowed with the norm: where for .

The functional-differential equations (22)-(23) include the meromorphic functions not belonging to . They were written ason the vector-function introduced in all by substitution (21) in the space . The operator and the given vector-function are determined by (22)-(23). Equation (28) was explicitly written in [11] as the system of functional-differential equations It was proved in [11] that the operator is compact in . One can see that the contrast parameter plays the role of the spectral parameter; hence, can be written in the form of power series in . This implies that the method of successive approximations applied to (29) converges in for sufficiently small . Let , () be a solution of (29). This unique solution belongs to . The given vector-function is twice differentiable in the closures of . Hence, the pumping principle [9, page 22] can be applied as follows. The shifts in composition operators of the right part of (29) are the shift strictly into domains. Hence, if we substitute , into (29), we obtain that , are twice differentiable in the closures of . The equivalent method of successive approximations can be applied to (22)-(23) more conveniently in computations.

The functions and are determined through and up to additive constants. For instance,

#### 4. Method of Successive Approximations

Application of successive approximations to functional equations is equivalent to Schwarz’s method described at the end of Section 2. It follows, for instance, from the uniqueness of the analytic expansion in near zero. Moreover, each iteration for the functional equations corresponds to an iteration step in Schwarz’s method since the coefficients in the series in are also uniquely determined. It can be also established directly form formulae written below.

Using the series (11) for and analogous series for other functions and applying successive approximations to the functional equations we obtain the following iteration scheme. The zeroth approximation is The next approximations for are where denotes the Kronecker symbol.

Introduce the functionsThen, It follows from (31) that can be written in the following form: where the following expansion is used: The th approximation for becomes and .

#### 5. Shear Modulus

##### 5.1. General Iterative Scheme

Introduce the average value over a sufficiently large rectangle containing all the inclusions : The averaged shear modulus of the considered finite composite is introduced as the ratio It is related to the effective shear modulus for macroscopically isotropic composites by the limit . It was demonstrated in [8] that (41) can be transformed into whereHere, is a solution to the problem with inclusions.

In order to determine , we first calculate the integral . Equation (37) implies that Application of (35) and Cauchy’s integral theorem yield The presented iterative scheme can be easily realized numerically. But we are interested in analytical formulae which can be obtained by symbolic computations. In the next sections, we perform symbolic computations to determine and the effective shear modulus in the third-order approximation.

##### 5.2. Second-Order Approximation

We are looking for in the form It follows from (37) that for the third-order approximation we need the integrals (45) for . Using the second equation (32), we have The functions are analytic in for . Therefore, the integrals with vanish in (47) by Cauchy’s integral theorem and (47) can be calculated by residues

In order to use (37) for we find from (34) Using the expansion for , we haveAlong similar lines Subtracting (51) and (52) we obtain Using the above formulae we obtain from (49) the exact formula:We are now ready to calculate the integral:

Using Cauchy’s integral theorem and residues we obtain This yields

##### 5.3. Third-Order Approximation

The third-order approximation requires advanced and long computations presented below. In order to calculate , we need the following function:It is obtained from (34) for by substitution given by (49) and calculated by (33) with .

Below, we describe general recurrent formulae for an arbitrary th approximation and explicitly write the third-order terms when . The following double series in and are used: The coefficients in the power series (61) are presented as series in : Substitution of (60)–(62) into (22) and selection of coefficients in the same powers of and yieldwith the zeroth approximation . Along similar lines, (23) yields with the zeroth approximation .

The expanded form of follows from (31):Equation (65) is in accordance with (37) whereUsing (66) we calculate the integral

The coefficients for can be explicitly written by the iterations (64):

The limit (43) has to be found. Using (44) and (67) we express through : Taking into account terms up to we rest for ; hence,

The above limits are calculated by use of the formalism developed in [8, 12]. It was supposed that equal nonoverlapping disks belong to a parallelogram (fundamental) cell periodically extended to the complex plane by two linearly independent translation vectors. As an example, we shortly present the transformation of the term of given by (68) multiplied by and complexly conjugated in accordance with (71): We are interested in the limit associated with the Eisenstein summation [8, 12]:The normalized -sums were introduced in [8, 12] by means of the Eisenstein summation: where . This means that the rectangle is normalized by the -linear transformation to having the unit area. Therefore, . Other terms are transformed by the same method. As a result we arrive at the following formula:where denotes the concentration. The absolute convergence of series in follows from the standard root test (Cauchy’s criterion).

The effective shear modulus is calculated by (42):whereExpansion of (79) in yields

#### 6. Numerical Simulations

The asymptotic formula (82) is a new theoretical formula obtained in the present paper. The computationally effective formulae and algorithms for the absolutely convergent sums and () were developed in [13, 14]. However, the numerical implementation of the conditionally convergent series (74)-(75) for and (76) for requires further investigations.

Formula (42) is similar to the famous Clausius-Mossotti approximation (Maxwell’s formula) [15, Section 10.4] applied for calculation of the effective conductivity of dilute composites. It is surprising that the Eisenstein summation and Maxwell’s self-consistent formalism are based on the different summation definitions of the conditionally convergent series [16, 17]. Using an analogy with the conductivity problem we now justify the proper limit value of , that is, (76) for . The Hashin-Shtrikman bounds [15, Ch. 23] for 2D incompressible elastic media become In the case , the bounds and are replaced with each other. One can check that the upper and lower bounds (83) coincide up to : This implies that the coefficients in the term of the expressions (82) and (84) must be equal. It follows from (80) that must vanish in the framework of the considered Maxwell’s formalism. The definition of is not essential in the final formulae since the terms with are cancelled in (81). The above demonstration is based on the formal pure mathematical arguments. Its physical interpretation has been not clear yet.

Consider a numerical example, the regular hexagonal lattice, when the -sums become the Eisenstein-Rayleigh lattice sums and calculated by algorithm presented in [8, 18]. Only the nonzero values of and are presented in Table 1.