Research Article | Open Access

Volume 2018 |Article ID 9230609 | https://doi.org/10.1155/2018/9230609

Wen Zhang, "The Elastic Solution of a Radial Heterogeneous Cylinder Subjected to Non-Uniform Distributed Normal and Tangential Loads", Mathematical Problems in Engineering, vol. 2018, Article ID 9230609, 8 pages, 2018. https://doi.org/10.1155/2018/9230609

# The Elastic Solution of a Radial Heterogeneous Cylinder Subjected to Non-Uniform Distributed Normal and Tangential Loads

Revised08 Apr 2018
Accepted07 May 2018
Published27 Jun 2018

#### Abstract

This paper presents an investigation of a cylinder with material attributes that vary arbitrarily in the radial direction under non-uniformly distributed normal and tangential pressures. A stress and displacement solution method for plane strain on a radial heterogeneous cylinder with inner and outer surfaces subjected to uneven normal and tangential pressures under two types of contact conditions (i.e., complete contact and smooth contact) is proposed based on the theory of elastic mechanics. In addition, a group of linear equations is derived, through which the analytical solution of a radial heterogeneous cylinder under a non-uniform load can be obtained. The validity of the analytical solution is verified by comparing it with the results of a numerical simulation. This research shows that the solution is more convenient and universal than traditional methods and can provide a theoretical basis for the stress state analysis, stability evaluation, and structure design of heterogeneous cylindrical structures, all of which have great significance in practical engineering.

#### 1. Introduction

Cylinders are important structures that are widely used in civil and mining engineering in addition to other engineering fields, and they are commonly implemented in machinery and national defense applications. Therefore, research on the stress and deformation of cylinders in their applications (e.g., for shaft linings and tunnels) has important value for cylinder design and safety evaluations.

The above-mentioned analytical solutions have achieved notable progress; however, those solutions are excessively complex and do not consider the comprehensive effects of different loads. Therefore, this paper proposes a mechanical model of a radial heterogeneous cylinder subjected to a new type of non-uniform load. The stress and displacement solution of the model is deduced in consideration of the contact conditions between osculant layers (complete contact and smooth contact) using elastic mechanics. In this paper, denotes the stress; and are the radial displacement and circumferential displacement, respectively; the subscripts , and represent the radial, circumferential, and shearing components, respectively; and the subscript (=1, 2, 3,  …, n; as below) indicates the number of the layers in the cylinder.

#### 2. Mechanical Model

##### 2.1. Nondimensionalization of Parameters

To generalize the solution, we select appropriate normalized variables to transform the parameters into dimensionless forms. Regular variables with units are expressed with a symbol.

The load is used to scale the relevant stress and pressure, and the inner radius of each layer is used to scale the displacement. The load is selected according to the conditions of different problems. For example, the vertical stress at the distal end of the formation is obtained by analyzing the shaft well or the tunnel lining.

, , and represent the dimensionless forms of the stresses, and represents the dimensionless form of the shear modulus .

and are the dimensionless displacements.

() and () are nondimensional coordinates.

##### 2.2. Mechanical Model

The pressure acting on the external cylinder can be expressed using a Fourier series dependent on the circumferential coordinates.

This study focuses on both parameter, which represents the uniform force that is self-balanced since the resulting value along the circumference is zero, and the cosine term, which is examined because of the similarity between the sine and cosine terms in the above equation. Moreover, the cosine terms are different; through analysis, the cosine term is self-balanced when , but the cosine term cannot balance itself when . Therefore, the distribution of the non-uniform load on the external cylinder is expressed as follows:where and reflect the non-uniform distributed normal load and tangential load, respectively, and , , and are the uniform and non-uniform distributed normal loads and the uneven tangential load, respectively. The tensile stress and outward radial displacement are positive according to the sign convention shown in Figure 1.

Figure 1 illustrates a force model of a radially inhomogeneous cylinder subjected to loads p and q. The radially inhomogeneous cylinder is regarded as an n-layered cylinder composed of several homogeneous and isotropically linear elastic layers. The inner and outer radii of the ith layer are and , respectively. The elastic modulus and Poisson’s ratio are and , respectively. The loads on the inner and outer surfaces are and and and , respectively.

#### 3. Model Solution

##### 3.1. Single-Layer Model Solution

Mechanical model I can be decomposed into many single-layer models (see Figure 2).

The analytic solution of the single-layer model is given as follows [1517]: where , , , through are unknown coefficients, is the non-dimensional radial coordinate, , and .

The stress boundary conditions of the single-layer model include , , , and . As these stress boundary conditions are applicable to arbitrary angles, they can be solved simultaneously with (4) and (6). The following six equations can therefore be obtained.

Furthermore, coefficients through can be determined by unifying the group of equations: where , , , , , , , and .

The dimensionless stress and displacement solutions for the single-layer model can be obtained by substituting (10) into (4) - (8).

##### 3.2. Solution for Mechanical Model I

Each individual layer in mechanical model I is normally subjected to one of two limited contact conditions, namely, a complete contact or a smooth contact.

###### 3.2.1. Complete Contact

In the case of complete contact, both the stresses and the displacements at the contact interface are continuous. Hence, according to the compatibility conditions of the displacements, the following equations are valid:where j=1, 2, 3,  …, n-1. Because the above boundary conditions are applicable to arbitrary angles , they can be simultaneously determined with (7) - (8). Thus, the following equations can be obtained.

Arranging (13) - (15), we can derive the following formulas:where , , , ,

Equations (16)-(18) comprise a -degree linear equation group with variables , , ,  …, , , and . These equations can be directly solved using mathematical calculation software. Then, substituting the results into the stress and displacement expressions of mechanical model I, the analytical solutions of stress and displacement for the complete contact condition can be obtained.

###### 3.2.2. Smooth Contact

In the case of smooth contact, the normal stresses and radial displacements at the contact interface are continuous, and the tangential stress is zero.

Therefore, the undetermined coefficients can be determined using (16)-(18); moreover, under this condition, and . Similarly, substituting these coefficients into the stress and displacement expressions of mechanical model I, the analytical solutions of stress and displacement for the smooth contact condition can be obtained.

#### 4. Engineering Example

The distributions of the temperature field, elastic modulus, and Poisson's ratio of a horizontal circular section of a frozen wall at a depth of 150 m are shown in Figure 3. The inner and outer radii of the frozen wall are 4.2 m and 10.2 m, respectively. The parameters of characteristic points within the frozen wall model are summarized in Table 1. The soil gravity is 0.02 MN/m3. The soil inside the frozen wall is excavated one layer at one time; therefore, the inner edge of the frozen wall is completely unloaded (, ). The external side of the frozen wall is subjected to a formation pressure with a lateral pressure coefficient of . The expressions for the stresses in polar coordinates are as follows.

 (m) Temperature (°C) Elastic Modulus (MPa) Poisson's Ratio 4.2 -12.5 393 0.27 6.8 -25 601 0.22 7.4 -25 601 0.22 10.2 0 219 0.33

The proposed solution method is used to analyze the distributions of the stress and displacement fields on the frozen wall.

The frozen wall is divided in the radial direction into a cylinder with 55 layers in complete contact according to the temperature distribution. Each layer is assumed to be a homogeneous isotropic elastic body. The flat part of the temperature distribution curve (6.8 m-7.4 m) in the middle of the frozen wall is considered a single layer with a thickness of 0.6 m, an elastic modulus of 601 MPa, and a Poisson's ratio of 0.22. The thickness of each remaining layer is 0.1 m, and the elastic moduli and Poisson's ratio values are obtained by linear interpolating the data shown in Figure 3 and Table 1.

Substituting the values of the physical and mechanical parameters of each layer into (16)-(18), the equations are then solved to obtain the forces and coefficients for every interface. Subsequently, by substituting the results into (4)-(8), the stresses and displacements of each layer can be determined. Thus, the stress and displacement fields of the entire frozen wall can be obtained.

To verify the results of the analytical solution, a finite element model consisting of one-quarter of the ice wall (0-) in consideration of its symmetry is established. The finite mesh elements are shown in Figure 4, where MPa, and the boundary constraint and force conditions are as follows.(1)Left boundary: sliding support restriction, the displacement in the x-direction being zero(2)Lower boundary: sliding support restriction, the displacement in the y-direction being zero(3)Inner boundary: acting loads and (4)Outer boundary: acting loads and

Figures 5, 6, and 7 indicate the distributions of the radial stress, radial displacement, and tangential stress, respectively, along both the direction of the minimum earth stress () and the direction of the maximum in situ stress () on the frozen wall. The values of the scattered points represent the results of the finite element calculations, and the curves represent the results of the theoretical calculations.

Figure 5 demonstrates that the radial stress nonlinearly increases in the radial direction and gradually transforms into the in situ stress.

As shown in Figure 6, a slight variation in the radial displacement is observed in the radial direction. The displacement in the direction of the maximum in situ stress () is much greater than that in the direction of the minimum earth stress (). This result indicates that the frozen wall experiences larger external expansion in the direction of the maximum in situ stress than in other directions.

Based on Figure 7, where , the tangential stress in the direction of the minimum earth stress () is much higher than that in the direction of the maximum in situ stress (). In the former case, the tangential stress decreases nonlinearly in the radial direction; moreover, in the latter case, the tangential stress initially increases nonlinearly and then decreases gradually in the radial direction.

Since the results shown in Figures 5, 6, and 7 are consistent with the finite element calculations, the correctness of the theoretical solution is verified.

#### 5. Conclusions

Radial heterogeneous cylinders subjected to asymmetric loads are often encountered in practical engineering. However, it is difficult to obtain the analytical solutions of the corresponding stress and displacement. Although previous studies have developed various solutions to this problem, those solutions are relatively complex and do not consider the comprehensive effects of different loads. Consequently, this paper proposes a stress and displacement solution method for the plane strain on a radial heterogeneous cylinder with inner and outer surfaces subjected to uneven normal and tangential pressures under two types of contact conditions (i.e., complete contact and smooth contact) based on the theory of elastic mechanics. In addition, a group of linear equations ((16)-(18)) is derived, through which the analytical solution for a radial heterogeneous cylinder under a non-uniform load can be obtained. Then, a finite element model of a horizontal circular frozen wall subjected to an uneven formation pressure is constructed to verify the correctness of the analytical solution, and the results indicate that the analytical solution is relatively universal and can be applied to realistic engineering applications involving cylindrical structures. Accordingly, the study provides a theoretical basis for the stress state analysis, stability evaluation, and structural design of cylindrical structures, all of which have great significance in practical engineering.

#### Data Availability

The data used to support the findings of this study are available from the corresponding author upon request.

#### Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

#### Acknowledgments

This work was financially supported by the National Hightech R&D Program of China (86-3 Program; no. 2012AA06A401) and the National Natural Science Foundation of China (nos. 41472224 and 41501075).

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Copyright © 2018 Wen Zhang. 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.