日本建築学会構造系論文報告集
Online ISSN : 2433-0000
Print ISSN : 0910-8025
ISSN-L : 0910-8025
379 巻
選択された号の論文の18件中1~18を表示しています
  • 原稿種別: 表紙
    1987 年 379 巻 p. Cover1-
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
  • 原稿種別: 表紙
    1987 年 379 巻 p. Cover2-
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
  • 原稿種別: 目次
    1987 年 379 巻 p. Toc1-
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
  • 原稿種別: 付録等
    1987 年 379 巻 p. App1-
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
  • 原稿種別: 付録等
    1987 年 379 巻 p. App2-
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
  • 山田 善一, 野田 茂
    原稿種別: 本文
    1987 年 379 巻 p. 1-14
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
    In this study, records obtained by the displacement-type seismographs of the Japan Meteorological Agency (JMA) were used because these seismographs have the most suitable instrumental characteristics in the period range between 2 and 20 sec. In order to examine the validity of JMA and SMAC records, we calculate the time history of ground displacement and acceleration response spectra during the Nihonkai-chubu earthquake of 1983, and compare them with the ones obtained from some other strong-motion seismographs. The displacement-time histories and response spectra calculated from the digitized seismograph records at three stations (Niigata, Akita and Tokyo) agree very well in the period range from 2 to 20 sec with the ones estimated from Omori's long-period strong-motion seismograph, acceleration and velocity-type strong motion seismographs having a wide dynamic range over a wide frequency range. These results seem to suggest that the JMA's displacement seismograms give a reliable and practical estimate in the period range of about 2 sec or longer, and are adequately available for their engineering purpose. When response spectra at four sites (Muroran, Hachinohe, Sakata and Akita) determined from SMAC accelerographs are compared with those from other kind of seismographs (JMA's displacement- and velocity-type seismographs), the former gives larger values for the period over about 5 sec than the latter. Following the study of Toki et al : (1986), its error depends on the shift and drift of the pen caused by a coupling between a deflect of the link and a friction between pen and paper. Futher study by the authors is underway for verifying the reliability of long-period component of SMAC and JMA's seismographs through a test on a shaking table. The paper will be published in forthcoming journal.
  • 壇 一男, 渡辺 孝英, 神田 順
    原稿種別: 本文
    1987 年 379 巻 p. 15-25
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
    An approximate representation of Wiener-Lee transform which describes the relation between Fourier amplitudes and phases of the minimum-phase-shift function is introduced in this paper. It is applied to the Fourier amplitudes of the earthquake ground motions to estimate the Fourier phases. The minimum-phase-shift functions are generated by the inverse Fourier transform of the amplitudes and the estimated phases. The results indicate that the complicated acceleration and velocity motions, such as those recorded in the epicentral regions of the 1979 Imperial Valley earthquake (M_L=6.6) or the 1983 Coalinga earthquake (M_L=6. 7), are quite different from the minimum-phase-shift functions. But their aftershock motions, with local magnitude of about 5. are similar to the minimum-chase-shift functions.
  • 石田 修三, 森迫 清貴
    原稿種別: 本文
    1987 年 379 巻 p. 26-33
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
    Many previous studies on simple K-braced frames suggest that the most efficient means to improve the overall toughness of K-braced multi-story steel frames are (1) to avoid the formation of collapse mechanisms on those beams supported by K-braces and (2) to prevent the early growth of yieldings on columns. In this paper, an efficient method of preliminary plastic design of multi-story K-braced steel frames is developed taking into account these two design requirements. A basic design factor ftj, the shear force ratio of bracings, is defined for the j-th story as the ratio of the story-shear-force to be assigned to the bracings to the prescribed design shear force of the story. Procedures of computing the vertical distributions of 0j are demon- strated. All the necessary informations for the preliminary plastic design can be easily derived from these fa values. A design example of ten-story three-bay K-braced frames shows that the method is very simple and effective to nrovide reasonable member sections?
  • 田中 尚
    原稿種別: 本文
    1987 年 379 巻 p. 34-37
    発行日: 1987/09/30
    公開日: 2017/12/25
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    In this paper, the author proposes a process to determine load and resisistance factors, especially for the case that safety margin consists of the terms each of which is composed of several random variables.
  • 市之瀬 敏勝, 滝口 克己, 吉井 正行
    原稿種別: 本文
    1987 年 379 巻 p. 38-48
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー

    Bi-directional hysteresis models are useful for dynamic response analyses of structures under two dimensional seismic excitation. The theory of plasticity for work hardening materials has been utilized for the bi-directional extension of uni-directional hysteresis models. The work softening (or strength degrading) hysteresis models are, however, difficult to be extended to bi-directional models by means of the theory of plasticity alone, because the theory utilizes Drucker's postulate of 'stable inelastic material'. This paper firstly presents a mathematical formulation to extend the uni-directional hysteretic model with work softening to bidirectional model. Secondly, this paper presents a series of earthquake response analyses to study the effects of work softening and bi-directional exitation on the seismic response. Following conclusions were obtained. (1) Hysteresis models with work softening can be classified into 2 types : (a) monotonic degrading type, in which the load-deformation relation by monotonic loading coincides with the envelope curve of the cyclic load-deformation relation as shown in Fig. 2, and (b) cumulative degrading type, in which the envelope curve of the cyclic load-deformation relation lies beneath the monotonic curve as shown in Fig. 1. (2) Restoring force-deflection relations of reinforced concrete members will be monotonic degrading type, if the strain of the centroids of the members does not exceed the strain at the compressive strength. Otherwise, the restoring force-deflection relations will be cumuratiye degrading type. (3) The fracture potentional defined on the deflection plane enables to extend the uni-directional hysteretic model with work softening to bi-directional model. (4) Assuming the expansion rule of the fracture potential as shown in Fig. 18 or 19 enables to express the cumurative degrading type or monotonic degrading type, respectively. (5) The virtual restoring force is defined as the actual restoring force minus the fracture portion of the restoring force. The plastic potential defined on the virtual restoring force plane enables the plastic potential to move and contract during the fracturing. (6) The proposed model agrees with the plane-section-remain-plane analysis of reinforced concrete sections. (7) The response of work softening system under either uni-directional or bi-directional earthquake exitation tends to go to one particular direction much more than that of work hardening system. (8) In the cases of work hardening system, the ratio of the uni-directional ductility response to the hysteretic energy absorbed is larger than that of the bi-directional one. In other words, the ductility response of the work hardening system by an uni-directional earthquake excitation is larger than that by a bi-directional earthquake excitation with the same amount of energy input. (9) In the cases of work softening system of the ratio of cumulative degrading type, the uni-directional ductility response to the hysteretic energy absorbed is larger than that of the bi-directional one. In other words, the ductility response of, the work hardening system by an uni-directional earthquake excitation is larger than that by a bi-directional earthquake excitation with the same amount of energy input. (10) The amount of energy input by earthquake excitation to work softening systems is about the same as that to work hardening systems. (11) The 'effective repetition number : N, is defined by N=E/Q_OD_y(μ-1) where E is the hysteretic energy absorbed by the system, μ is the yield strength of the system, D_y is the yield defletion of the system, and ju is the maximum ductility reponse of the system during the earthquake. The number, N, can be approximated as the function of the ratio of K_2K_1 or K_3/K_1 as shown by the solid line or the broken line in Fig. 27. This approximation as well as the assumption of same amount of

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  • 石井 透, 神田 順, 岩崎 良二
    原稿種別: 本文
    1987 年 379 巻 p. 49-57
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
    Many works have been carried out in order to examine the phase characteristics of earthquake ground motions for the improvement of earthquake resistant design of building structures. Especially the phase difference distribution has lately attracted considerable attentions as it approximately determines the envelope of time history. This paper examines phase characteristics of recorded motions and their effects on the response spectra by use of the phase difference concept, and discusses the role of phase characteristics which should be considered in simulating motions. The standard deviation of phase differences, σ_<ΔΦ>, for components in a narrow frequency band was found to be considerably less than that for all components. It was also revealed that only the representation of σ_<ΔΦ> is not sufficient to express the phase characteristics of motions in terms of the peak acceleration, Amax, the envelope shape and response characteristics. Then, the narrow band phase difference tendency is cons- idered to be applied in simulating motions. A method of generating artificial ground motions with consideration for phase characteristics in narrow frequency ranges is proposed in this paper. Fourier phases are derived from phase differences generated with consideration for phase characteristics in narrow frequency ranges. The standard deviation of phase differences in a narrow frequency band is set to be about 0.75 times of that for all components which is supposed to be equal to σ_<ΔΦ> of recorded motions. Simulated motions according to the proposed method were confirmed to posess Amax, σ_<ΔΦ> and response spectra satisfactorily close to those of recorded motions.
  • 玉井 宏章, 近藤 一夫, 末岡 禎佑, 花井 正実
    原稿種別: 本文
    1987 年 379 巻 p. 58-70
    発行日: 1987/09/30
    公開日: 2017/12/25
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    In this paper, four new rectangular plate bending models for the finite element method based on the modified principle of potential or complementary energy are proposed. These models have special features as follows. 1) The displacement parameter on a node of the structural system in the analysis is only the nodal deflection. 2) The displacement fields of a element and its boundary are expressed as a function of the displacement parameters of the nodes, not only in its element but also in the adjacent elements, so that they could have the higher order displacement functions without increasing the total number of displacement parameters. 3) The displacement functions of the elements and their boundaries are obtained in the explicit expression. 4) The continuity requirements on inter-elements are satisfied by using the modified variational principle. The deflections and resultant stresses of rectangular thin plates are calculated in order to examine the convergencies and accuracies of the present models. Also, the behavior of flat slabs under uniformly distributed load is investigated as a practical example. As a result of the analyses, it may be concluded that these present models are very useful for reducing the total number of the unknown displacement parameters.
  • 三谷 勲, 今門 一弘
    原稿種別: 本文
    1987 年 379 巻 p. 71-78
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
    Empirical formula for plastic rotation capacity of H-shaped steel beam-columns (Eq. (7)) is established based on the test results in Refs. 4) and 5). Factors used in the formula are width to thickness ratios of flange and web, lateral unbraced length, ratio of end-moments, yield stress of the steel, axial load ratio, and coefficient of effective lateral buckling length. Comparison of predicted values with experimental results (Refs 2), 4)〜6)) indicates that the empirical formula Eq. 7) is sufficient to estimate the plastic rotation capacity of steel beam-columns with H-shaped cross section for practical use. The ranges of factors used in the comparison are as follows : 8<6/f<16, 17<D/ω<70, 17<l_b/i_y<110, 0<P/P_y<0.6, -0.8<M2_/M_1<0, 2.7<σ_y<8.4 (tf/cm^2) where 2 b = flange width, D = depth of the cross section, f and ω=thicknesses of flange and web respectively, i_y= radius of gyration about weak axis of the cross section, σ_y = yield point of the steel, P = axial load, P_y = yield axial load, and M_1, and M_2=unequal end-moments. Appricability of the formula to beam-columns in a rigid frame is discussed. It is found that the proposed formula based on the rotation 8 in Fig. 1 can apply to estimation of the plastic rotation capacity of beam-columns defined by using the rotation r in Fig. 1.
  • 島本 明, 児玉 道正, 山村 正明
    原稿種別: 本文
    1987 年 379 巻 p. 79-90
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
    Forced vibration tests were performed with small-scale model silos on a shaking table in order to evaluate the dynamic effective mass during vibration of cylindrical silos used for storing granular materials. Four general conclusions were drawn I 1) For a given ratio of height to diameter (H/D), ranging from 0. 5 to 2.5, the measured resonance frequencies of a model silo filled with storage materials are 15-20 % those of the silo when it is empty. 2) As excitation acceleration amplitude increases, peak acceleration amplification values of contained material decrease and shift to lower frequencies. This was also mathematically simulated by a numerical analysis which expressed the shear modulus and damping ratio as a function of strain. 3) Resonance frequencies of silos are proportional to the square root of extensional rigidity, independent of the type of fill material. This is approximated by the vibration of a continuous solid when a silo's H /D is less than 3. 4) When a silo's extensional rigidity is below a certain constant value, the coefficient of dynamic effective mass is unity. If H/D>1.5, this coefficient is approximately 1.0, and if H/D<1, the coefficient is approximately 0.5-1. 0.
  • 岸田 英明, 上杉 守道, 椿原 康則
    原稿種別: 本文
    1987 年 379 巻 p. 91-92
    発行日: 1987/09/30
    公開日: 2017/12/25
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  • 徳富 久二
    原稿種別: 本文
    1987 年 379 巻 p. 92-93
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
  • 原稿種別: 付録等
    1987 年 379 巻 p. App3-
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
  • 原稿種別: 表紙
    1987 年 379 巻 p. Cover3-
    発行日: 1987/09/30
    公開日: 2017/12/25
    ジャーナル フリー
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