Missouri University of Science and Technology Scholars' Mine International Conference on Case Histories in Geotechnical Engineering (1988) - Second International Conference on Case Histories in Geotechnical Engineering Jun 1st On Properties of Damping of Bases Wang Xikang Central Research Institute of Building & Construction of MMI, China Follow this and additional works at: http://scholarsmine.mst.edu/icchge Part of the Geotechnical Engineering Commons Recommended Citation Xikang, Wang, "On Properties of Damping of Bases" (1988). International Conference on Case Histories in Geotechnical Engineering. 14. http://scholarsmine.mst.edu/icchge/2icchge/2icchge-session4/14 This Article - Conference proceedings is brought to you for free and open access by Scholars' Mine. It has been accepted for inclusion in International Conference on Case Histories in Geotechnical Engineering by an authorized administrator of Scholars' Mine. This work is protected by U. S. Copyright Law. Unauthorized use including reproduction for redistribution requires the permission of the copyright holder. For more information, please contact [email protected]. Proceedings: Second International Conference on Case Histories In Geotechnical Engineering, June 1-5, 1988, Sl Louis, Mo., Paper No. 4.07 On Properties of ·Damping of Bases Wang Xlkang Senior Engineer, Central Research lnsl of Building & Construction, Ministry of Metallurgical Ind., Beijing, China SYNOPSIS: On the basis of many tests it has been proved that the damping properties of bases not only Have bearing on magnitude of base area of foundation but also on weight of foundation and on mecha~ nics model adopted. This paper puts forward the computation formulas of damping parameters to some soils. iNTRODUCTION dynamic rigidity, damping coefficient and soil mass must be determined the model may be referred to as three parameter model. The reasonableness of adopting three parameter model had been discussed in detail in the paper 2 and is not discussed herein. In order to compute the vibration response of structures and foundations under machinery with satisfactory precision it is necessary to establish the damping properties of bases correctly. In recent years the problem above mentioned has been researched by the author and his colleagues under the conditions of field tests employing vertical forced vibration with smaller amplitude which were performed on foundation of different sizes and different soil conditions. When researching the damping properties of bases a new concept is cited, Whereby the mass participating in foundation vibration includes not only mass of foundation but also soil mass. In consequence of considering the soil mass not 0 nly the damping parameters established agree wi~h practice to a ~reater exterit but also the precision of computation of vibration reaponse acquires great improvement. In the following several main results of research are introduced in detail. Under the harmonic vertical exciting force with constant amplitude as shown in Fig.l the equation of motion of foundation may be written as follows: Pzsinwt Fi&'·l Vibration llodel m Considerin&' Sol I lless 1. MECHANICS MODEL AND THEORETICAL FORMULAS FOR DAMPING COMPUTATION ( 1) Before researching the damping properties of bases the mechanics model of foundation vibration must be first developed because using the different mechanics model wil1 obtain different dynamic parameters. When analysing the damping properties of bases, the model of Mass-Damping-Spring of linearity is adopted as shown in Fig.l and the following assumptions are employed: · 1) Base soils . possess not only elasticity but also inertia effect. 2) The soil mass participating in vibration and vertical damping coefficient as well as veitical dyna*ic rigidity of bases are not varied within the range of •xciting fre~uen cies. where: m and m = Mass of foundation ~nd soil s Maximum value and frequency of exciting force c Vertical damping coefficient Dynamic • rigidity · of · base K z z Verticil displacement - cif · foun~ dation Limiting our discussion to forced vibration merely, we take the solution of the question in the form: Z = A z Sfn( . Co) . t - 9) where: Az= Amplitude of vibration 9 :, Phase shift In order to obtain three dynamic parameters we Because three dynamic parameters which are Second International Conference on Case Histories in Geotechnical Engineering Missouri University of Science and Technology http://ICCHGE1984-2013.mst.edu ( 2) 765 Second International Confer Missouri University of Scienc http://ICCHGE1984-2013.ms Second International Confer Missouri University of Scienc http://ICCHGE1984-2013.ms ~;::.:::::: •::·:. :::·::.:::::: :-··· ~~~_: ::::::·!:=:!:~:-:::::·:::::: :::::::.::•. ·~ .__:_M_:,_,:._:~ ...:.:--. :*:;·t~~ i~::r::rrr:: .... :::·.:·::.::.::·:::::·.::::.::::::::::."'" : •.. ·:tf¥:-:::::::~::::::·:.:: :.::;·.:::.::-:::.::::, Second International Confer Missouri University of Scienc http://ICCHGE1984-2013.ms :;;··· · ·r=:
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