{"title":"Annual index vol 4, 1984","authors":"","doi":"10.1016/0261-7277(84)90040-8","DOIUrl":"https://doi.org/10.1016/0261-7277(84)90040-8","url":null,"abstract":"","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 4","pages":"Page 222"},"PeriodicalIF":0.0,"publicationDate":"1984-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90040-8","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"137441096","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Elastic-plastic buckling of buried pipelines by seismic excitation","authors":"L.N.H. Lee, T. Ariman, C.C. Chen","doi":"10.1016/0261-7277(84)90032-9","DOIUrl":"10.1016/0261-7277(84)90032-9","url":null,"abstract":"<div><p>A quasi-bifurcation theory of dynamic buckling and a simple flow theory of plasticity are employed to analyze the axisymmetric, elastic-plastic buckling behavior of buried pipelines subject to seismic excitations. Using the seismic records of the 1971 San Fernando earthquake, a series of numerical results have been obtained, which show that, at strain rates prevalent in earthquakes, the dynamic buckling axial stress or strain of a buried pipe is only slightly higher than that of static buckling.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 4","pages":"Pages 168-173"},"PeriodicalIF":0.0,"publicationDate":"1984-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90032-9","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"74585344","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Dynamic structure - soil interaction under the action of vertical ground motion, Part II: the plane problem","authors":"X. Zeng , A.S. Cakmak","doi":"10.1016/0261-7277(84)90037-8","DOIUrl":"10.1016/0261-7277(84)90037-8","url":null,"abstract":"<div><p>For a strip wall erected on a rigid strip foundation and supported on the surface of the ground, the dynamic structure-soil interaction under the action of the vertical ground motion is investigated. The ground motion is idealized as vertically propagating, vertical steady-state motion. For the contact between the foundation and the ground, two cases are considered: (a) the contact is perfectly smooth; (b) the contact is assumed to be welded along the contact surface beneath the foundation. The use of Fourier and Laplace transform methods yields dual integral equations (for the case without friction) or simultaneous dual integral equations (for the case with welded contact). Both of them are solved by means of infinite series of orthogonal functions, the Jacobi polynomials. The displacement of the foundation, the response of the system to the incident excitation, and the distributions of contact stresses beneath the foundation are presented. The numerical results show that there are significant differences between the relative displacements of the top of the wall with respect to its base, for the cases of smooth and welded contact.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 4","pages":"Pages 211-219"},"PeriodicalIF":0.0,"publicationDate":"1984-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90037-8","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"88885751","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Effect of repeated loading on the strength of clay","authors":"Ergün Togrol, Erol Güler","doi":"10.1016/0261-7277(84)90034-2","DOIUrl":"10.1016/0261-7277(84)90034-2","url":null,"abstract":"<div><p>The behaviour of soils under dynamic loading conditions has been studied. There exists a large amount of data indicating that a reduction of strength in a soil takes place but that the amount of this reduction is limited. On the other hand some authors claim that such a reduction is not possible because the ultimate undrained shear strength of a given saturated soil depends only on its void ratio and structure. In this paper it is attempted to bring some clarification to this conflict and in doing so the Critical State Model is employed. Fifty-eight dynamic and nine static triaxial tests have been conducted on samples consolidated from a water content twice the liquid limit to different consolidation pressures. The soil used in experiments is ‘Arnavutköy Kaolini’ with a liquid limit of <em>w</em><sub><em>L</em></sub> = 65% and plastic limit <em>w</em><sub><em>P</em></sub> = 30%. The results of the present series of tests indicate that the main effect of dynamic loading is on the increase of the pore water pressure which in turn causes the soil to behave like an overconsolidated soil. Previous research has shown that the void ratio of an overconsolidated soil sample decreases at the shear zone during shearing. All the results expressed above, as well as the results of tests conducted during this research, indicate that a reduction in the shear strength occurs in a normally consolidated clayey soil due to the repeated loading application.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 4","pages":"Pages 184-190"},"PeriodicalIF":0.0,"publicationDate":"1984-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90034-2","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"74488782","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Dynamic structure - soil interaction under the action of vertical ground motion, part I: the axisymmetric problem","authors":"X. Zeng , A.S. Cakmak","doi":"10.1016/0261-7277(84)90036-6","DOIUrl":"10.1016/0261-7277(84)90036-6","url":null,"abstract":"<div><p>In the epicenter area, the acceleration for the vertical component plays an important role in the anti-seismic design. Supposing that a rod is erected on a rigid circular foundation, and the foundation is supported on the surface of the ground, the dynamic structure-soil interaction under the action of the vertical ground motion is investigated. The ground motion is typically idealized as vertically propagating, vertical steady-state motion and the ground is idealized as a linear, homogeneous, isotropic elastic half-space. For the contact between the foundation and the ground, two cases are considered: (a) the contact is perfectly smooth, namely, there is no shear stress on the contact surface; (b) the contact is assumed to be welded along the contact surface. The use of Hankel and Laplace transform methods yields respectively for the two cases dual integral equations or simultaneous dual integral equations. Both of them are solved by means of the infinite series about some orthogonal function. For the three cases of rigid ground, smooth contact, and welded contact, results are presented for the response of the structure-soil system to the incident excitation. For the cases of smooth and welded contacts, the stress distribution along the bottom surface of the foundation is investigated.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 4","pages":"Pages 200-210"},"PeriodicalIF":0.0,"publicationDate":"1984-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90036-6","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91519691","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"International conference on Natural rubber for earthquake protection of building and vibration isolation 1982","authors":"","doi":"10.1016/0261-7277(84)90047-0","DOIUrl":"https://doi.org/10.1016/0261-7277(84)90047-0","url":null,"abstract":"","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 3","pages":"Page 165"},"PeriodicalIF":0.0,"publicationDate":"1984-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90047-0","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91958979","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Response of hammer foundations to pulse loading","authors":"L. El Hifnawy, M. Novak","doi":"10.1016/0261-7277(84)90042-1","DOIUrl":"10.1016/0261-7277(84)90042-1","url":null,"abstract":"<div><p>The response of hammer foundations to the blows of the head can be considered either as caused by the initial velocity imparted to the anvil or as a pulse. This paper presents a solution based on the latter assumption. The approach is based on the notion of complex eigenvalues, incorporates damping in a rigorous way and is particularly suitable for more complex types of hammer foundations featuring more than one degree of freedom.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 3","pages":"Pages 124-132"},"PeriodicalIF":0.0,"publicationDate":"1984-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90042-1","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"86839342","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Ranjit S. Dhaliwal, B.M. Singh, J. Vrbik, A.P.S. Selvadurai
{"title":"Diffraction of torsional wave or plane harmonic compressional wave by an annular rigid disc","authors":"Ranjit S. Dhaliwal, B.M. Singh, J. Vrbik, A.P.S. Selvadurai","doi":"10.1016/0261-7277(84)90045-7","DOIUrl":"10.1016/0261-7277(84)90045-7","url":null,"abstract":"<div><p>In this paper we have considered the following two problems. Firstly the diffraction of normally incident <em>SH</em> waves by a rigid annular disc situated at the interface of two elastic half-spaces is considered. The solution of the problem is reduced into the solution of triple integral equations involving Bessel functions. The solution of the triple integral equations is reduced into Fredholm integral equations of th second kind. By finding the solution of the Fredholm integral equation, the numerical values for the moment required to produce the rotation of disc are obtained. Secondly, the problem of diffraction of plane harmonic compressional wave by an annular circular disc embedded in an infinite elastic space is considered. The annular disc is assumed to be perfectly welded with the infinite solid. The solution of the problem is reduced into the solution of Fredholm integral equation of the second kind. The Fredholm integral equation is solved numerically and the numerical values for the couple applied on the disc are obtained.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 3","pages":"Pages 150-156"},"PeriodicalIF":0.0,"publicationDate":"1984-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90045-7","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"86130053","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Soil amplification: some refinements","authors":"Eduardo Kausel, JoséM. Roësset","doi":"10.1016/0261-7277(84)90041-X","DOIUrl":"10.1016/0261-7277(84)90041-X","url":null,"abstract":"<div><p>The most widely used techniques for the study of one-dimensional amplification of vertically propagating seismic waves involve solution of the dynamic equations in the frequency domain with linearly viscoelastic material properties. Material nonlinearities are approximately modeled by iterative use of linear solutions, adjusting values of modulus and damping until they are compatible with computed levels of strain. The program SHAKE is the best known example of a code using this procedure.</p><p>Several refinements to the iterative scheme originally proposed by Seed and Idriss are presented in this paper. In particular, it is shown that the solution for the layers underlying the control motion can be obtained in one single step, when the mass matrix is diagonal. Use of the shear stress in place of the shear strain as the controlling parameter in determining material properties gives faster convergence and identifies cases of potential non-convergence. Trivial modifications are also proposed to the standard scheme that would enable the researcher to study the amplification or deconvolution of non-vertically incident <em>SH</em> waves with a code like SHAKE. These modifications consist simply in changing the mass density of the soil, and redefining the characteristic strain.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 3","pages":"Pages 116-123"},"PeriodicalIF":0.0,"publicationDate":"1984-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90041-X","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76415593","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Deconvolution method between kinematic interaction and dynamic interaction of soil-foundation systems based on observed data","authors":"Masaru Hoshiya, Kiyoshi Ishii","doi":"10.1016/0261-7277(84)90046-9","DOIUrl":"10.1016/0261-7277(84)90046-9","url":null,"abstract":"<div><p>To prove the effect of kinematic interaction experimentally, earthquake records both at the ground and at the foundation are needed. Since the foundation motion is effected not only by the kinematic interaction but also by the dynamic interaction of a soil-foundation system, a general deconvolution method between the kinematic interaction and the dynamic interaction of a soil-foundation system based on the observed data is derived in this paper, where a structure is modelled by a multiple-degree-of-freedom (MDOF) system which represents the dynamic interaction, and the unknown foundation input motion is expressed by a moving average model (MA-model) of the ground motion, which represents the filtering effect of kinematic interaction. Generally, as the parameters of a MDOF system can not be determined exactly, these parameters are treated as random variables on trial using the Monte Carlo simulation method. Next, the coefficients of the MA-model are identified applying the Kalman filter. On the many trials, the result which minimizes the root-mean-square error between the observed response and calculated response is determined as the best estimation. Examples of (1) two single-degree-of-freedom systems arranged in a series and (2) a four-storey reinforced concrete school building are demonstrated to verify the proposed method.</p></div>","PeriodicalId":100715,"journal":{"name":"International Journal of Soil Dynamics and Earthquake Engineering","volume":"3 3","pages":"Pages 157-164"},"PeriodicalIF":0.0,"publicationDate":"1984-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0261-7277(84)90046-9","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78320138","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}