Abstract
Consider a homogeneous and isotropic elastic plate of thickness h o = const > 0, which occupies a region \( \bar Sx[ - h_0 /2,h_0 /2] \) in ℝ3, where S is a domain in ℝ2 with a simple, closed boundary ∂S. In the transverse shear deformation model proposed in [1] it is assumed that the displacement vector at (x 1, x 3), x = (x 1, x 2) ∈ ℝ2, at time t ≥ 0, is of the form
where the superscript T denotes matrix transposition. Then the vector u = (u 1, u 2, u 3)T satisfies the equation of motion
here B = diag{ρh 2, ρh 2, ρ}, h2 = h 2 0/12, ρ is the plate density, ∂ t = ∂/∂t,
∂α = ∂/∂x α, α = 1,2, λ and µ are the Lamé constants satisfying λ + µ > 0 and ε > 0, and q is a combination of the forces and moments acting on the plate and its faces x 3 = ±h 0/2.
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References
C. Constanda, A mathematical analysis of bending of plates with transverse shear deformation, Pitman Res. Notes Math. Ser. 215, Longman/Wiley, Harlow-New York, 1990.
I. Chudinovich and C. Constanda, Nonstationary integral equations for elastic plates, C.R. Acad. Sci. Paris Sér. I 329 (1999), 1115–1120.
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Chudinovich, I., Constanda, C. (2004). Time-Dependent Bending of a Plate with Mixed Boundary Conditions. In: Constanda, C., Largillier, A., Ahues, M. (eds) Integral Methods in Science and Engineering. Birkhäuser, Boston, MA. https://doi.org/10.1007/978-0-8176-8184-5_8
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DOI: https://doi.org/10.1007/978-0-8176-8184-5_8
Publisher Name: Birkhäuser, Boston, MA
Print ISBN: 978-1-4612-6479-8
Online ISBN: 978-0-8176-8184-5
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