Journal of Structural and Construction Engineering (Transactions of AIJ)
Online ISSN : 2433-0000
Print ISSN : 0910-8025
ISSN-L : 0910-8025
Volume 397
Displaying 1-18 of 18 articles from this issue
  • Article type: Cover
    1989 Volume 397 Pages Cover1-
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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  • Article type: Cover
    1989 Volume 397 Pages Cover2-
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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  • Article type: Cover
    1989 Volume 397 Pages Cover3-
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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  • Article type: Appendix
    1989 Volume 397 Pages App1-
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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  • Article type: Appendix
    1989 Volume 397 Pages App2-
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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  • KAZUO SUZUKI, YOSHITERU OHNO, SOMNUKE PRAPARNTANATORN, HAJIME NINOMIYA ...
    Article type: Article
    1989 Volume 397 Pages 1-11
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    1. Introduction Almost every code of concrete structural design relates permissible crack width to exposure conditions, indicating the general agreement about the influence of crack on corrosion. The relationship between crack width and corrosion, however, has not been clarified. The locations of steel corrosion normally coincided with tips of flexural cracks revealing the indisputable effect of crack on corrosion initiation. It also appeared that steel was not corroded at every crack. In addition, the effect of crack on corrosion propagation is remarkably perplexed. With the same surface crack width, the deterioration of steel corrosion can range from zero to high degree of corrosion. The study aims to clarify the mechanism of corrosion induced by crack and the relationship between crack width and corrosion by using an electrochemical technique. 2. Experimental Procedures The Specimens and loading arrangement are shown in Fig. 1. The designation and steel stress of the specimens are tabulated in Table 1. The steel reinforcement was one D 13 millscale bar. The mix proportion and strength properties of concrete are shown in Table 2. Two levels of flexural crack width were introduced and sustained under tensile steel stresses of 2000 and 3000 kg/cm^2. Steel corrosion was accelerated by subjecting the specimens to repeated cycles of one day wetting in 65℃, 3.1 % NaCl solution and one day drying under room environment. Exposure periods are also shown in Table 1. During the exposure test, Half cell potential (E_c) and Polarization resistance (R_p) of steel were periodically measured against a Ag/AgCl reference electrode and a platinum counter electrode. The specimens were split at the end of their exposure periods to observe corrosion situations such as corrosion form, corroded length and rusted area. 3. Results and Discussion 3.1 Locations of Crack and Rust Fig. 2 shows the locations of crack and rust. All rusted areas were associated with crack tips as they were reported. The aggressive substances essential for corrosion processes, such as Cl^-, H_2O, O_2 etc., can undoubtly penetrate through crack easier than through sound cover. However, it was also found that, steel did not corrode at every crack as presented in the literature 3.2 The electrochemical characteristics Fig. 3 shows the typical distribution of E_c and R_p, measured at various exposure ages, along four locations of four specimens. After a period of exposure, in each specimen, one of the four locations remarkably showed the higher reduction in Ec and Rp values comparing to other three locations. Corrosion was certainly found under these spots (see specimens S (3, 2) and L (1, 1)). Fig. 4 shows the typical E_c and R_p time curves. The Ec negative shift revealed the depassivating period after the amount of absorbed chloride ions had exceeded the critical value of C1^-/OH^<-20>). During the depassivating, although all points of the specimens altogether shifted to more negative potentials, only R_p of the corroding spots declined continuously. R_p of the uncorroded spots slightly increased with time. For specimens with more than one corroded spot, the corroding order of the corroded spots can be determined by their R_p characteristics (see specimens S (4, 1) and L (4, 1)). 3.3 The electrochemical characteristics and corrosion situations The comparison of average electrochemical values of corroding and uncorroded spots, measured at various locations, is shown in Fig. 5. Both corroding and uncorroded spots had the same trend of E_c with time. The actual E_c of the uncorroded spots might be defected by the presence of E_c of the corroding spots. In contrast with E_c time curve, the corroding and uncorroded spots had clearly different trend of R_p with time. The R_p of the corroding spots continuously shifted to more negative values, whilst the R_p of the uncorroded spots tended to increase gradually. The active

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  • AKIKO MORI, YASUNORI MATSUFUJI
    Article type: Article
    1989 Volume 397 Pages 12-18
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    Extrusion experiments were carried out with mortars of which fine aggregates had different geometries but a same particle size distribution. The mortars were prepared to various water contents, and extruded at several rotational speeds of screw. Both extruding pressure and velocity were measured. Graphic analyzer was used to measure fine aggregate geometries which correlated well with extrusion characteristics. That is, the more spherical the configuration of fine aggregate was, the lower the extruding pressure was, but the higher the velocity was. At comparatively low water content ratios, influences of fine aggregate geometry on the extruding velocity were a little, but much on the pressure. At the higher water content ratios, the effects could not be observed so obviously. Extruding pressure and velocity have been generally thought to be prescribed by the extruder operating point which is determined by a cross point of screw characteristics and die characteristics. This concept may be also applied to the mortars with various fine aggregate geometries. And the die characteristics of screw extrusion were found to be similar to those of piston extrusion. The extruding pressure was directly proportional to the shearing stress of mortar, but the extruding velocity was inversely. It is suggested that the shearing stress of mortar is used for a substitute of Y and τ_<R0> in Eq. 1 presented by Benbow.
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  • HIROZO ISHIKAWA
    Article type: Article
    1989 Volume 397 Pages 19-31
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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  • TAKASHIGE ISHIKAWA, KYOKO HIRATA
    Article type: Article
    1989 Volume 397 Pages 32-41
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    The Draft Bills of Tokyo City Building Ordinance, planned by Dr. Yorinaka Tsumaki since 1889, were repealed, but they played an important role in the history of building law. The structural regulations in them have characteristics as follows: 1) For the first time, Dr. Tsumaki introduced the regulations about iron frames, the earthquake-proof regulations on a building built of brick and stone into these draft bills. 2) These draft bills were referred to a large number of foreign building code. These draft bills didn't imitate all of them, but these draft bills also had their own originality. 3) These draft bills were partially referred to the next Draft Bills of Tokyo City Building Ordinance planned by members of A. I. J. . But the questions how they were selected, remain.
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  • HIROSHI KATUKURA, TAKAHIDE WATANABE, YASUHIRO HAYASHI, TEIJI TANAKA
    Article type: Article
    1989 Volume 397 Pages 42-47
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    This paper presents an idea of the processing of strong motion accelerograms considering causality of seismic waves. It is presented that, by the technique of FFT shown in Fig. 1, and by considering causality condition shown in Fig. 2, permanent displacements with some errors (in this paper, we call such displacements as drifts) can be obtaind even from accelerograms. The flowchart to calculate the drifts is indicated in Fig. 3. Examples of the drifts are shown in Figs. 7 and 8. For Imperial Valley earthquake, 1979, the calculated drift components can well explain the permanent displacements deduced from the fault motion.
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  • KOJI MORITA, KAZUMASA EBATO, AKIYUKI FUNAHASI, TADAYOSHI KOMINAMI, TAK ...
    Article type: Article
    1989 Volume 397 Pages 48-59
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    Structural behaviors of beam-to-column connections has scarcely been studied when the corner weld of box-column section is partial penetration weld. In this study, connection assemblage tests have been carried out with variables of throat thickness of corner weld, plate thickness of inner diaphragm, and, layout and size of beam flange. And the conclusions attained are as followings. 1) Maximum shear strength of corner weld at connection panel increases with throat thickness of corner weld and plate thickness of inner diaphragm, and it depends on the layout of beam flange to corner weld. 2) Yield, general yield and maximum strengths of corner weld at connection panel can be estimated by Eq. (5), (8) and (9), respectively. 3) General yield and maximum strengths of beam end joint can be estimated by Eq. (15) and (16), respectively when wide flange beam is welded to box column. And they are almost independent of the throat thickness of corner weld.
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  • KOJI YODA, KATSUHIKO IMAI, YOSHIAKI KUROBANE, KOJI OGAWA
    Article type: Article
    1989 Volume 397 Pages 60-72
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    Pre-fabricated large-span building frames with rigid conections are economically designed by using thin-walled H-sections as their members. Under gravity load conditions, the strength of members forms a ruling factor in the design of these frames. Under the influence of strong earthquake motions, however, the deformation capacity of members is another decisive factor in controlling the maximum responses of these structures. For members that are braced against lateral deflection, the evaluation of the rotation capacity of the members after local buckling is a subject that remains to be solved for the seismic design of these structures. This paper discusses effects of local buckling on moment-rotation hysteretic behavior of thin-walled welded H-section beams that are simply supported and under a concentrated load on the center. Specimens are fully braced against lateral deflection and are tested in either monotonic or cyclic loading. The variables in the specimens are width-thickness ratios of flanges and webs, whose values are varied as follows; b/f=9-15 H/ω=60-180 in which b denotes the half width of the flange ; f, the thickness of the flange ; H, the depth of the cross section ; and ω, the thickness of the web. The following are observations from monotonic loading tests. The moment capacity of sections immediately decreases to 95-85 % of its maximum value as a result of local buckling of the flanges. After the load decay, moment-rotation curves show a gradual decrease in moment capacity as a further rotation is imposed until the beams sustain large deflection. The hysteretic behavior as follows was observed from cyclic loading tests. Hysteresis loops show a remarkable decrease in capacity during early stages of cyclic loading. However, the capacity degradation turns out insignificant after applying 4-5 cycles of loading. In conclusion simple empirical formulas for predicting moment-rotation relationships of these sections are proposed based on the existing test results.
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  • SHUZO ISHIDA, KIYOTAKA MORISAKO
    Article type: Article
    1989 Volume 397 Pages 73-82
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    This paper introduces a numerical method which is able to predict with good accuracy the elastic-plastic behavior of plane skeletal structures. This method, called FERT-P, is a combined and integrated version of the following two methods. One is the combined geometrically and materially nonlinear one-dimensional finite element method proposed by Nakamura, Ishida and further developed by the authors (Refs. 2-7), which has recently been called PERT (Finite Element method with Rigid-body-motion coordinates and Transfer matrix technique). The other is the incremental perturbation method developed by Nakamura, Uetani et al. (Refs. 8-11) to provide means of finding every point on an equilibrium path at which a new element will start yielding or unloading. The incremental perturbation method is able to determine automatically computational step lengths. Several benchmark tests have been carried out on the elastic-plastic buckling of steel structures. The following conclusions for the FERT-P have been derived: (1) By adopting the rigid-body-motion coordinates, the perturbation calculation in the FERT-P is concerned only in the transformation of global and local coordinates. The development of the FERT-P program is very easy. (2) The transfer matrix technique is effective for deriving the perturbation equations of members from those of elements. (3) The FERT-P is a very reliable numerical method to analyze elastic-plastic behaviors, including in particular the unstable behavior, of plane skeletal structures.
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  • AKIHIKO KAWANO, CHIAKI MATSUI
    Article type: Article
    1989 Volume 397 Pages 83-90
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    Strength of lateral-torsional buckling of a truss is influenced by the position of transverse loads which act on the nodal point of the truss except laterally stiffened supports. If the transverse loads act on the top chord of the truss, the buckling strength is reduced because of additional torsional moments due to the transverse loads. This paper presents the influence of the transverse loads on the lateral-torsional buckling of various truss types by elastic and inelastic buckling analyses. From the results, we make clear that lateral-torsional buckling moments of tubular trusses are hard to be affected by the transverse loads in comparison with H-shaped beams, and the buckling moments of the trusses under various loading conditions are always equal to or larger than the buckling moments under uniform bending. In addition, we propose a more rational and simple design method for the lateral-torsional buckline of tubular trusses subjected to transverse loads.
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  • KOICHIRO HEKI, MASUMI MURAKAMI, KAZUMI YAMANE
    Article type: Article
    1989 Volume 397 Pages 91-103
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    This paper is concerned on the in-plane elastic buckling behavior of double-layer rigid-jointed latticed two-hinged arches subjected to asymmetrical radial load. To treat the problem simply and analytically, the approximate calculation method by the continuum treatment using the effective strength and the effective rigidity is presented considering the geometrical nonlinearity being expressed by the perturbation method. Based on some examples of numerical analysis treated in this paper, the following conclusions are drawn. 1) The in-plane buckling load of lattice arches under asymmetrical loading is smaller than that under symmetrical loading as well as the case of continuum arches. 2) In case of lattice arches under symmetrical loading, overall buckling mode or member buckling mode appears at the critical point. The former is antisymmetrical configuration and the latter is member buckling at the middle portion of the arch where the sectional forces are in the critical state. While, in case of lattice arches under asymmetrical loading or antisymmetrical loading, member buckling occurs at the portion of the arch where the sectional forces are in the critical state. In which, the phrase "the sectional forces are in the critical state" means that equilibrium paths of sectional forces intersect with the surface of the effective strength in the sectional forces space. Thus, on in-plane buckling of lattice arches, member buckling is explained by the effective strength and overall buckling by the effective strength and/or the effective rigidity. 3) The fundamental and post buckling equilibrium paths of lattice arches under symmetrical loading calculated by the present continuum treatment method agree with those by the discrete treatment method considering the finite displacement. 4) The value of buckling load obtained by present method using the effective strength and the effective rigidity fairly well agrees with the value obtained by the discrete treatment method considering the finite displacement. Thus, the applicability of the present method by the continuum treatment is verified for the calculation of the load and the mode of in-plane elastic buckling of lattice arches.
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  • KOICHIRO HEKI
    Article type: Article
    1989 Volume 397 Pages 104-110
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
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    This paper is dealt with the in-plane elastic buckling of the circular ring which is supported by uniformly distributed springs in tangential directions and subjected to three types of external pressure. The acting directions of three types of loads after buckling are constant, normal to the surface and centripetal, respectively. The main conclusions are as follows. 1) The buckling mode is of a cos nθ type for the normal displacement, sin nθ for tangential displacement, and also sin riff for the rotation of section unless coupling terms between shear and others exist. 2) The effect of stretching strain on the buckling load is negligible small on the order of EI≪EAγ^2. 3) The values of buckling load are expressed in simple formula ignoring the stretching strain, and the effect of shear deformation and coupling rigidity between shear and bending is made clear. 4) A pracical procedure to obtain the buckling load is presented. 5) For free rings without tangential support, the buckling load subjected to the pressure of constant direction is not the well known result, p_α=4EI/γ^3, but zero accompanying the mode of rigid body rotation.
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  • Article type: Appendix
    1989 Volume 397 Pages App3-
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
    JOURNAL FREE ACCESS
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  • Article type: Cover
    1989 Volume 397 Pages Cover4-
    Published: March 30, 1989
    Released on J-STAGE: December 25, 2017
    JOURNAL FREE ACCESS
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