Abstract
This paper investigates the application of a double Fourier series technique to the construction of an elastic stress field in a cylindrical bar subject to lateral boundary loads. The lateral loads, including the constant load boundary conditions, are represented by two Fourier series: one on the perimeter of the circular section (r 0, θ) and the other on the longitudinal curved surface parallel to the bar axis (z). The technique invokes acceptable potential functions of the Papkovich–Neuber displacement field, satisfying the governing partial differential equations, to assign appropriate odd and even trigonometric Fourier terms in cylindrical coordinates (r, θ, z). The generic solution decomposes the problem of interest to a state of stress caused by two independent boundary conditions along the z axis and θ-polar angle, both superimposed on a solution for which these potentials are the product of the trigonometric terms of the independent variables (θ, z). Constants appearing in the resultant second-order partial differential equations are determined from the generally mixed (tractions and/or displacements) boundary conditions. While the solutions are satisfied exactly at the ends of an infinite bar, they are satisfied weakly on average, in the light of Saint Venant’s approximation at the two ends of a finite bar. The application of the proposed analysis is verified against available elastic solutions for axisymmetric and non-axisymmetric engineering problems such as the indirect Brazilian Tensile Strength and Point Load Strength tests.
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Abbreviations
- L, r 0, D :
-
Half the length (width), radius and diameter of a laterally loaded cylinder, respectively
- E, ν :
-
Elastic Young’s modulus and Poisson’s ratio of the material
- e ijk :
-
The permutation or Levi-Civita symbol
- r, θ, z :
-
Polar coordinates with origin at the centre of a laterally loaded cylinder
- x, y, z :
-
Cartesian coordinates with origin at the centre of a laterally loaded cylinder
- \({\varvec{\epsilon}}\) :
-
Strain tensor
- \({\varvec{\sigma}}\) :
-
Stress tensor
- \(\user2 u\) :
-
Displacement vector
- μ, λ :
-
Lamé’s constants
- u, v, w :
-
Components of displacement vector
- \(\bar{{\mathbf I}}\) :
-
Identity matrix
- tr():
-
Trace of a given matrix
- \({\left(\right)}^{\rm T}\) :
-
Transpose of a given matrix
- (),j :
-
The comma in a subscript denotes the derivative symbol, i.e. \(( )_{,j} =\frac{\partial ( )}{\partial x_{j} }\)
- \(\user2{F}\) :
-
Body force vector
- x i :
-
Coordinate directions
- δ ij :
-
The Kronecker delta
- π :
-
The ratio of circle’s perimeter over its diameter
- σ rr , σ θθ , σ zz :
-
Radial, transverse and axial stress components in cylindrical coordinates
- σ r θ , σ θ z , σ rz :
-
Shear stress components in cylindrical coordinates
- σ xx , σ yy , σ xy :
-
Components of stress tensor in Cartesian coordinates
- ∇, ∇., ∇× :
-
Gradient, divergence and curl operators, respectively
- ∇2 :
-
Laplace operator
- \({\varvec{\psi}}\) :
-
Harmonic vector potential
- ϕ :
-
Harmonic scalar potential
- R :
-
The position vector
- ψ r , ψ θ , ψ z :
-
Components of a harmonic vector in cylindrical coordinates
- \(\beta, \gamma, \zeta \) :
-
Frequencies of the lateral load in axial direction of a cylinder
- η :
-
A constant equals or greater than 4
- f :
-
Either the stress or displacement distributions at the surface of a cylinder, i. e. \(u_{r(r=r_{0} )} \) or \(\sigma _{rr(r=r_{0} )}\)
- \(I_{m} (\zeta _{n} r)\) :
-
The modified Bessel function of the first kind of order m and the non-negative argument \(\zeta _{n} r\)
- m, n :
-
Integer numbers
- P :
-
Total load per radial length applied on the lateral curved surface of a cylinder
- S :
-
Total load applied on the lateral curved surface of a cylinder
- p :
-
The applied radial surface stress in Brazilian problem
- p′, q′:
-
The interior and exterior radial stresses in the 2D circular hollow disc of the Lamé problem
- a′, b′:
-
The inner and outer radii in the 2D circular hollow disc of the Lamé problem
- f(n, r), g(n, r), h(n, r):
-
Functions of n and r only in cylindrical coordinates
- f(m, n, r), g(m, n, r), h(m, n, r):
-
Functions of m, n and r only in cylindrical coordinates
- b :
-
Half the width of the applied pressure in the strip loaded problem and also in the point load test
- α :
-
Half the loading angle in both Brazilian and point load problems
- t :
-
The thickness of the Brazilian disc
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Acknowledgments
The first author acknowledges two scholarships, granted by the Commonwealth Scientific and Industrial Research Organization (CSIRO) and The University of Queensland (UQ): (i) Minerals Down Under Flagship Scholarship of CSIRO (CESRE), and (ii) UQ Postgraduate Scholarship from the School of Civil Engineering at UQ. The authors also acknowledge the valuable discussions with Professor Emmanuel Detournay, of the University of Minnesota, on the subject.
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Serati, M., Alehossein, H. & Williams, D.J. 3D Elastic Solutions for Laterally Loaded Discs: Generalised Brazilian and Point Load Tests. Rock Mech Rock Eng 47, 1087–1101 (2014). https://doi.org/10.1007/s00603-013-0449-9
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DOI: https://doi.org/10.1007/s00603-013-0449-9