Abstract
The stability problems of clamped skew plates are considered with the inplane stresses represented in terms of oblique components. Deflection is expressed in terms of a double series of beam characteristic functions of clamped-clamped beam. Energy method is used to obtain buckling coefficients under individual loadings and for a few cases of combined loading. Convergence is examined in a few representative cases. For buckling in shear, two critical values exist the magnitude of negative shear being much larger than that of positive shear.
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Abbreviations
- a, b :
-
dimensions of the plate
- C rs :
-
coefficient in the series expansion of deflection
- D :
-
flexural rigidity of the plate (Eh 3/12(1−v 2))
- E :
-
Young's modulus of the material of the plate
- G, H (1),H (2),H (3) :
-
matrices defined in (15)
- G 1 :
-
matrix defined in (16)
- h :
-
plate thickness
- I pqmr , J pqns :
-
integrals defined in (11)
- K :
-
order of the matrix
- M, N :
-
maximum number of terms inx- andy-directions respectively
- N x,N y,N xy :
-
midplane forceshσ x,hσ y,hσ xy respectively
- \(\bar R_x^* ,\bar R_y^* ,\bar R_{xy}^* \) :
-
nondimensional midplane force parameters,\(\frac{{h\sigma _x a^2 \cos ^3 \psi }}{D},\frac{{h\sigma _y a^2 \cos ^3 \psi }}{D},\frac{{h\sigma _{xy} a^2 \cos ^3 \psi }}{D}\) respectively
- \(\bar R_x ,\bar R_y ,\bar R_{xy} \) :
-
buckling coefficients,\(\frac{{\sigma _x hb^2 }}{{\pi ^2 D}},\frac{{\sigma _y hb^2 }}{{\pi ^2 D}},\frac{{\sigma _{xy} hb^2 }}{{\pi ^2 D}}\) respectively
- U :
-
strain energy of the plate
- V :
-
potential energy of the middle surface forces
- W(ξ, η):
-
deflection of the plate
- X m(ξ),Y n(η):
-
beam characteristic functions
- x, y, z :
-
oblique coordinate system defined in Fig. 1
- x 1,y 1,z :
-
orthogonal coordinate system defined in Fig. 1
- ξ, η :
-
nondimensional coordinates,x/a andy/b respectively
- ν :
-
ratio
- σ x,σ y,σ xy :
-
oblique stress components defined in Fig. 1
- λ :
-
side ratio (a/b)
- ψ :
-
skew angle
- ▽ 2 :
-
skew differential operator\(\left( {\sec ^2 \psi \left( {\frac{{\partial ^2 }}{{\partial x^2 }} - 2\sin \psi \frac{{\partial ^2 }}{{\partial x^2 \partial y}} + \frac{{\partial ^2 }}{{\partial y^2 }}} \right)} \right)\)
- ▽ 21 :
-
skew differential operator in nondimensional coordinates\(\left( {\sec ^2 \psi \left( {\frac{{\partial ^2 }}{{\partial \xi ^2 }} - 2\lambda \sin \psi \frac{{\partial ^2 }}{{\partial \xi ^2 \partial \eta }} + \lambda ^2 \frac{{\partial ^2 }}{{\partial \eta ^2 }}} \right)} \right)\)
- α, β :
-
ratios ofσ y/σ x andσ xy/σ x respectively
- ε m,ε n :
-
beam eigenvalues, (7) and (8)
- α m,α n :
-
parameters in beam characteristic functions, (7) and (8)
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Prabhu, M.S.S., Durvasula, S. Stability of clamped skew plates. Appl. Sci. Res. 26, 255–271 (1972). https://doi.org/10.1007/BF01897854
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DOI: https://doi.org/10.1007/BF01897854