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Optimal versions of braced girder used in civil engineering, by Finite Element Method
MIHAI NEGRU, VILCU ROSCA, ADRIANA IONESCU Faculty of Mechanics University of Craiova
ROMANIA , .
Abstract: This paper presents two optimized versions of a steel structure used in civil engineering obtained thru a process of structural optimization using Finite Element Method. The main advantage of these optimized structures is the cost which is 50% smaller then the cost of a standard version of this steel structure. The optimization process was made using Finite Element Method and Ansys program. The paper presents the results of structural optimization process and the static analysis of these optimized steel structures in two load cases: the snow weight and the seism simulation.
KeyWords: Finite Elements Method, Steel Structure, Civil Engineering, Structural Optimization, Ansys
1 Introduction Steel offers much better compression and tension than concrete and enables lighter construction. Steel structures use threedimensional trusses, so they can be larger than reinforced concrete counterparts. Computerized, highprecision stress analysis and innovative jointing allow an array of structures and shapes. Steel frame construction now predominates. Examples include the 200meter Astro/Dome and Super Dome in the United States and Japan's Fukuoka and Nagoya domes. This paper analyze the steel structures used for manufacturing buildings. These buildings are made from I section beams with large dimensions of the I section (78cm x 26cm), as in figure 1.
Fig.1 The present version of the steel structure
This kind of structure has multiple disadvantages because the weight of the steel is bigger and the welding process is difficult. So, the costs of these types of structures are bigger then it should be. Basically the optimization process, in this case, consists in improving a initial shape of the braced girder and the columns which sustain it. This searching was made by making different types of structural modifications of shapes and improving those which had a good behavior at snow and seismic loads. These behaviors were determined using linear structural static analysis in Ansys program. The initial shape of the braced girder, which was subjected to the process of structural optimization is presented in fig.2.
Fig.2 The initial shape of the braced girder
Proceedings of the 10th WSEAS International Conference on MATHEMATICAL and COMPUTATIONAL METHODS in SCIENCE and ENGINEERING (MACMESE'08)
ISSN: 1790-2769 364 ISBN: 978-960-474-019-2
2 Problem Formulation The overall equilibrium equations for linear structural static analysis are:
or
where: [K] = total stiffness matrix u = nodal displacement vector N = number of elements [F r ]= reaction load vector [F a ], the total applied load vector, is defined by:
where: [F nd ] = applied nodal load vector [F ac ] = [M]ac = acceleration load vector [M] = total mass matrix ac = total acceleration [F th e ] = element thermal load vector [F pr e ] = element pressure load vector For our case the two load cases are the snow weight and the seismic load:
Uk Gs G S ⋅ + ⋅ + ⋅ = 05 , 1 5 , 1 35 , 1 Uk Gs G E ⋅ + ⋅ ⋅ + ⋅ = 05 , 1 5 , 0 5 , 1 35 , 1
where: S – snow load; G – the weight of the steel structure including the roof E – seismic load; Gs – the weight of the snow (2000 N/m 2 ) Uk – the effect of the structure exploitation
Uk = 0,75 [N/m 2 ]
3 Problem Solution The initial shape of the braced girder subjected to the process of optimization has an opening of 15 m and the height of the two columns of 4 m. The structure optimization steps are presented below. The results of static analysis of the braced girder are presented only on half of the structure because of the geometric symmetry.
Fig. 3 First version of the braced girder
Fig.4 – Von Mises stress for the first version
Fig. 5 Second version of the braced girder
Fig.6 – Von Mises stress for the second version
Fig.7 – Von Mises stress for the third version
Proceedings of the 10th WSEAS International Conference on MATHEMATICAL and COMPUTATIONAL METHODS in SCIENCE and ENGINEERING (MACMESE'08)
ISSN: 1790-2769 365 ISBN: 978-960-474-019-2
Fig. 8 Forth version of the braced girder
Fig.9 – Von Mises stress for the forth version during snow case load
Fig.10 – Von Mises stress for the forth version during seism case load
For the forth version in the snow case load the Von Mises stress is uniformly distributed over the entire structure and the maximum value is 200MPa. The same situation is achieved during the seism load.
Fig. 11 Forth version of the braced girder
Fig.12 – Von Mises stress for the forth version during snow case load
Fig.13 – Von Mises stress for the forth version during seism case load
The fifth version has the advantages of the forth versions but the values of Von Mises stress in both load cases are a little bit higher. The maximal values of the stress are distributed on bigger areas.
Proceedings of the 10th WSEAS International Conference on MATHEMATICAL and COMPUTATIONAL METHODS in SCIENCE and ENGINEERING (MACMESE'08)
ISSN: 1790-2769 366 ISBN: 978-960-474-019-2
Both optimized versions (forth and fifth) are made by beams with small sections: 40mm x 30mm x 2mm 15mm x 15mm x 1,5mm 20mm x 20mm x 1,5mm 60mm x 40mm x 2mm. The joint of the beams is made by welding.
4 Conclusion The optimization process has been successful and the final two versions of the braced girder (forth and fifth) can be used for steel structures. The analysis for the optimized structures show that the fifth version of braced girder has a little bit less rigidity then the forth version but is using less material because it is manufactured using only 3 trusses. Both optimized versions of braced girders have good behaviors for both load cases (snow and seism) and they can replace the standard steel structures which use heavy beams with large dimensions I sections. The main advantage of these lighter optimized versions is: 50% smaller costs because the weight of the steel structure is 3 times smaller then the standard structure, so we use 3 times less steel!
References: [1] Negru M., Rinderu P., Manea I, Spectrum analysis of the SF6 High Voltage Circuit Breaker using Finite Element Method, The XIII International Congress on Sound and Vibration, ICSV13, CD ROM Proceedings, Vienna 2006, Austria
[3] M. Negru, Dumitru N., Rinderu P., Modal analysis of the SF6 high voltage circuit breaker using finite element method, The XIII International Congress on Sound and Vibration, ICSV 12, CD ROM Proceedings, Lisbon 2005, Portugal. [4] O.C. Zienkiewicz, R.L. Taylor, The Finite Element Method, Fourth edition, V.2, McGraw Hill. [5] *** Ansys User’s Guide [6] Negru M., Rinderu P., Curtu I. – Modal analysis of the portal plane milling machine optimized resistance structure by using F.E.M. , The XII International Congress on Sound and Vibration, ICSV12, 1114 july, Lisabona, Portugalia, 2005 [7]Negru M., Bolcu D.,Manea I. Earthquake simulation of the SMEP 400kV high voltage disconnector structure using Finite Element Method, 11th WSEAS International Conference on COMPUTERS (July 2628, 2007) Crete Island, Greece. [8]Negru M., Curtu I. Design optimization of the resistance structure of the portal plane milling machine using F.E.M., bulletin of Faculty of Mechanics Iasi, Romania, 2004, ISSN 10112855 [9] Negru M., Georgescu I., Albota E., Optimization of a large steel truss structure used in civil engineering, by Finite Element Method, 1st WSEAS International Conference on FINITE IFFERENCES FINITE ELEMENTS FINITE VOLUMES BOUNDARY ELEMENTS (September 1113, 2008) Malta.
Fig.14 – The final version of the steel structure using optimized braced girders
Proceedings of the 10th WSEAS International Conference on MATHEMATICAL and COMPUTATIONAL METHODS in SCIENCE and ENGINEERING (MACMESE'08)
ISSN: 1790-2769 367 ISBN: 978-960-474-019-2