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Civil-Comp Proceedings
ISSN 1759-3433 CCP: 88
PROCEEDINGS OF THE NINTH INTERNATIONAL CONFERENCE ON COMPUTATIONAL STRUCTURES TECHNOLOGY Edited by: B.H.V. Topping and M. Papadrakakis
Paper 26
Analytical Calculation of Composite Beams According to Second Order Theory M. Aminbaghai and R. Binder
Institute for Structural Analysis, Vienna University of Technology, Austria M. Aminbaghai, R. Binder, "Analytical Calculation of Composite Beams According to Second Order Theory", in B.H.V. Topping, M. Papadrakakis, (Editors), "Proceedings of the Ninth International Conference on Computational Structures Technology", Civil-Comp Press, Stirlingshire, UK, Paper 26, 2008. doi:10.4203/ccp.88.26
Keywords: second order theory, transfer matrix method, transfer functions, critical load, continuous variable Young's modulus, continuous variable shear modulus.
Summary
Based on [1] a calculation concept for structures with composite beams according to
Second Order Theory can be presented. The cross-sections of the beams are
constant, but the Young's Modulus E and the Shear-Modulus G can be variable
along the length of the beam.
The bending stiffness EI, the extensional stiffness EA and shear-stiffness GA~ have been described by polynomials of arbitrary degree. The special case of constant stiffness is included in the general case. The distribution of the Young's Modulus is continuous. In the special case of a discontinuity in the Young's modulus' distribution, the beams can be spilt in two or more sections with a continuous distribution. The beam is calculated due to uniaxial bending. The axial force NII according to Second Order is constant and for the special case of First Order Theory it is zero. Line loads can be described by polynomials of arbitrary degree. The special loads for Second Order Theory are also included in this concept. The thermal load Delta T can be considered by a constant curvature kappae = Delta T * alphaT/h. alphaT is the coefficient of thermal expansion and h is the depth of the beam. First of all the differential equation for the lateral displacement w is derived. This differential equation of third degree can be solved using the Mathematica program. The solutions of the governing differential equations are used to present the moment M and the shear force Q. The present calculation concept has been subjected to numerical testing on a single-beam-construction considering a variable bending stiffness EI, a variable extensional-stiffness EA and a variable shear stiffness GA~. The static program IQ 100 [2] can be used for calculations of beams with variable bending stiffness EI and variable extensional-stiffness EA, but without shear stiffness effect GA~=infinity. In this case the results of the present calculation concept can be verified by the static program IQ100 and the critical load for that case can be gained too. References
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