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Membrane Stress Field and Eigenvalue Problems at Rotating Circular Plates of Small Thickness, in Thermal Regime

机译:膜应力场和特征值在旋转圆形板上的小厚度,热状态下

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From the analytical equations study of the disks behavior, some very important issues yield, issues which will be analyzed and solved in the following research. In the present paper one takes into account the fact that the study of the static and dynamical bending subjected disks, most be done mostly under the existence of a membrane stresses field (rotational motion, temperature field with a nonuniform distribution along the radius etc.). In the case of a plate of constant thickness, one uses the equation below: DΔ~2w + ζ(w) + ρh((partial deriv)~2w)/((partial deriv)t~2) = q, (1) where: w - the displacement measured normal to the plate's plane; q - the distributed force, normal to the plate's plane; D = Eh~3/12(1-v~2) - cylindrical modulus of elasticity, at bending of the plate; Δ - Laplace's operator; v - Poisson's ratio; h - the thickness of the plate; ρ - the material density.
机译:从分析方程研究磁盘行为,一些非常重要的问题产量,在以下研究中将分析和解决的问题。在本文中,考虑到静态和动态弯曲的磁盘的研究,大多数大多数在膜应力场(旋转运动,沿半径不均分布的温度场)的存在下进行的。在恒定厚度板的情况下,使用以下等式:dδ〜2w +ζ(w)+ρh((部分deriv)〜2w)/((部分deriv)t〜2)= q,(1)其中:W - 板平面正常测量的位移; Q - 分布力,平面正常; D = EH〜3/12(1-V〜2) - 弹性弹性模量,在板的弯曲时; δ - 拉普拉斯的操作员; V - 泊松比例; h - 板的厚度; ρ - 材料密度。

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