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APPROACH FOR THE SOLUTION OF A SIMPLIFIED REISSNER THEORY OF ELASTIC PLATES - APPLICATION IN THE AUTOMOTIVE INDUSTRY- ICSAT 2010 1.

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Presentation on theme: "APPROACH FOR THE SOLUTION OF A SIMPLIFIED REISSNER THEORY OF ELASTIC PLATES - APPLICATION IN THE AUTOMOTIVE INDUSTRY- ICSAT 2010 1."— Presentation transcript:

1 APPROACH FOR THE SOLUTION OF A SIMPLIFIED REISSNER THEORY OF ELASTIC PLATES - APPLICATION IN THE AUTOMOTIVE INDUSTRY- ICSAT 2010 1

2 2 Motivation Benefits of modern Plate-Theories:  More accurate stress and deformations analysis  New Elements in FEM (shape functions )  Weight reduced, optimized structures Sustainability R EISSNER Theory:

3 3 Classic plate theory Kirchhoff`s Theory: 4th order differential equation based on Kirchhoff`s assumption Solution well-known (e.g. FE-Solvers) practical and fast solutionScope: - Very thin plates, stiff plates - Transverse shear rigid plates

4 4 Innovative materials Laminates, sandwich materials etc. Characteristics like: Thicker plates relatively soft interlaminar shear modulus High Safety Factor  Oversized Constructions Problems:  Kinematic Hypothesis based on B ERNOULLI /K IRCHHOFF is not adequate  Imperfection on the boundaries

5 Modern plate theory of R EISSNER Key points: 1. Hypothesis of stress distribution:  Stress in plane is identically to the K IRCHHOFFS Theory  Transverse shear stress  Normal transverse stress 5 Three dimensional state of stress

6 Modern plate theory of R EISSNER 6 Basic assumptions Geometrically linear: small strains, small displacements (Theory of first order) Constitutive linear elastic equation (H OOKE ’s law) Isotropic/orthotropic Materials behavior Rectangle coordinates for polygon plates 2. Virtual Work Principal:  Deflection w  Two averaged rotations (normal to the mid-plane of plate) Defining resultant strain quantities (fictitious)

7 The dynamic governing equations 7  Systems of three inhomogeneous, transient, linear, partial, coupled Differential Equations of 6 th order with constant coefficients  12 Constant of Integration  three independent boundary conditions The first R EISSNER differential equation The second and third R EISSNER differential equation Problem: No solution yet

8 Assumption: A very small imperfection of the elastic plate (G AUSS curvature ) 8 Introduction of hypothesisCoupling-Term Uncoupling Solution possible with common methods

9 Load type specification Distributed Load: Polynomial function: Symmetrical or non symmetrical pressure for rectangle plates (time invariant and no smoothing terms ) 9

10 Particular Integral: Comparison of Coefficients Homogeneous Solution: Identical to K IRCHHOFF Theory Superposition First Reissner differential equation: 4th order: 8 free constant for adjustments on the boundaries 10 Analytical solution: static problem

11 11 Analytical solution: static problem Second Reissner differential equation Second Reissner differential equation (Analogous for the third equations): 2nd order: Homogeneous solution provides four constants of integration Superposition: 11 Uncoupling General Solutions consist of 16 constant of Integration …well known, analytical Functions: superposition’s of hyperbolic and trigonometric terms, power series approach and recursive formulas

12 Natural Stone Laminate. Derivation of transversal isotropic R EISSNER Equations  The difference is assumed to be neglectable Homogenization 12 Orthotropic Material - A directionally dependent, inhomogeneous Composite:

13 13 Prospect 13 Modified Reissner equations  Integrals for three differential equation could be derivate separately  Enough Variables for adjustments on the boundary Parameter study: Effects of the assumptions Investigation on H OOKS Law and Homogenization Validity Conclusion Higher degree of accuracy in stress analysis  Weight reduced, optimized Structures


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