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Civil-Comp Proceedings
ISSN 1759-3433 CCP: 81
PROCEEDINGS OF THE TENTH INTERNATIONAL CONFERENCE ON CIVIL, STRUCTURAL AND ENVIRONMENTAL ENGINEERING COMPUTING Edited by: B.H.V. Topping
Paper 187
Non-linear Three-Dimensional Analysis of the Charles Bridge Exposed to Temperature Impact J. Šejnoha, J. Zeman, J. Novák and Z. Janda
Department of Structural Mechanics, Faculty of Civil Engineering, Czech Technical University in Prague, Czech Republic , "Non-linear Three-Dimensional Analysis of the Charles Bridge Exposed to Temperature Impact", in B.H.V. Topping, (Editor), "Proceedings of the Tenth International Conference on Civil, Structural and Environmental Engineering Computing", Civil-Comp Press, Stirlingshire, UK, Paper 187, 2005. doi:10.4203/ccp.81.187
Keywords: Charles bridge, historical structures, temperature impact, two-scale analysis, water flow-structure interaction.
Summary
The Charles bridge in Prague is one of listed monuments having a
paramount historical importance. On 9th July 1357 in the morning,
exactly at 5 hours and 31 minutes, which corresponds to the numerical
sequence 135797531, Charles IV of the Louxenbourg Dynasty, King of
Bohemia and Germany and Italy, Roman Emperor, laid the foundation stone
and entrusted Peter Parlér and his stone mason's workshop to
construct the bridge. Currently, a living discussion of two groups of
specialists is underway on the concept of the bridge repair in the
Czech Republic. The discussion mainly revolves around the function and
performance of the reinforced concrete slab put in the bridge during
the reconstruction in 1966-1975. It speaks for itself that the repair
of the Charles Bridge is extremely demanding professionally, and,
besides, carefully watched by the society as a whole. Therefore, detailed
analyses of the response of the bridge to loading impact appears to be
inevitable. It is obvious that they should be carried out on cogent
material models and using progressive computational techniques.
This paper is a continuation of our previous works [1,2,3]. These papers deal with special material models related to quarry masonry and to natural stone masonry distinguished itself by regular and/or irregular geometry, respectively. The quarry masonry fills up the inner part, while the natural stone masonry forms the vertical surfaces and the vault of the bridge. In the framework of two-scale numerical homogenization, two different scales of analysis are considered - the mesoscopic (mesostructural) level, where a typical dimension is related to the size of the stone block, and the macroscopic level at which the bridge is analyzed as a whole. The typical feature of the homogenization-based approach on the mesoscopic scale is that all the non-linear calculations are performed on a periodic unit cell (PUC). The present paper utilizes specific applications of these techniques to the evaluation of effective material properties described in the accompanying papers [4,5] and in references therein. On macroscopic scale, the analysis is carried out on the three-dimensional segment of the bridge. The fracture energies are determined as areas under the loading curves derived on the mesoscopic scale and multiplied by the width of the localization band. This approach is of course a certain simplification of reality. Nevertheless, it can be realized immediately with the help of existing software ATENAWin [6] including the non-linear character of the problem linked to the evolution of cracks, which can be correctly represented. The macroscopic calculations are conducted in two steps. In the first step, the non-stationary simultaneous moisture and heat transport is analyzed in a characteristic cross-sections of the bridge. The courses of the temperature calculated at individual material points complies well with the results of in situ measurements using temperature and moisture sensors. In the second step, the response of a bridge segment to temperature impact is analyzed under the assumption of periodic repetition of the bridge segments (vaults). Finally, incorporation of an additional load due to the bridge-water flow interaction is considered as a next logical step in moving the numerical model closer to reality. References
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