Journal of the Japanese Society for Experimental Mechanics
Print ISSN : 1346-4930
ISSN-L : 1346-4930
Volume 9, Issue 4
Displaying 1-11 of 11 articles from this issue
Original Articles
  • Tatsuro WAKIMOTO, Kenji KATOH
    Article type: Original Article
    2009Volume 9Issue 4 Pages 318-323
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    Three-dimensional deformation and merging of disturbance waves in a radial liquid sheet has been clarified. The radial liquid sheet is generated when flowing liquid film on a disk emerges radially from the disk edge. The radial liquid sheet is unstable because of a velocity profile with an inflection point (inflectional instability). The growth and deformation of the two-dimensional disturbance waves (D waves), which is formed by the instability, lead to laminar-turbulent transition just outside of the disk edge. In this study, the deformation process of the D waves was observed in detail with a CCD camera providing high temporal and spatial resolution images. Comparing the observed deformation of the D waves with the reported typical deformation of vortices formed by inflectional instability in a single-phase free shear flow, three-dimensional deformations of the D waves and vortices were very similar. This suggests that three-dimensional deformation of the D waves is caused by enhancement of perturbed vortex filament in a braid region. However, merging of the D waves hardly occurred even though vortices in the free shear flow merge frequently. This implies that existence of liquid surface prevents the merging of the D waves.
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  • Tatsuro WAKIMOTO, Kenji KATOH, Mituyoshi HIGASHINE
    Article type: Original Article
    2009Volume 9Issue 4 Pages 324-329
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    A new optical measurement method for detection of slight difference of contact angle has been developed. This new method is applied to detect the micro blemish of self assembled monolayers (SAMs) because the blemished SAMs causes slight difference of contact angle from that of normal SAMs. In this method, a test plate is preliminarily set up at a tilt angle, which is same as the contact angle of normal SAMs. This setting forms a very small two-dimensional meniscus near the plate depending on the contact angle difference between blemished SAMs and normal SAMs. When a laser beam is emitted to the meniscus from above, the incident laser beam is reflected at a certain angle depending on the inclined angle of the liquid surface formed by the meniscus. In consequence, the contact angle difference is measured based on the reflection angle of the laser beam. This method is capable of detecting slight angle difference under 1 degree between blemished SAMs and normal SAMs.
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  • Tatsuro WAKIMOTO, Kenji KATOH
    Article type: Original Article
    2009Volume 9Issue 4 Pages 330-337
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    Nonlinear growth of disturbance waves in a radial liquid sheet has been clarified. The radial liquid sheet was formed by releasing of a radial water film flowing along the disk into still air. In this liquid sheet, a velocity profile with an inflection point is formed during the relaxation of the velocity profile. This velocity profile causes inflection point instability, and the instability amplifies disturbances in the liquid sheet. The deformed liquid surface by the amplified disturbance produces disturbance waves. In this study, the growth of the disturbance waves depending on the amplitude of the wave was analyzed by numerical simulation and experiment. The thickness and surface velocity at the disk edge were selected to be 80μm and 14.2m⁄s, respectively. The disturbance waves with different amplitudes were numerically simulated, and the simulated disturbance waves demonstrated that the growth rate decreases when the amplitude exceeds 15μm, which is 19% of the sheet thickness. In addition, the comparison of measured amplitude by the laser reflection method with that of the simulated disturbance waves revealed that the amplitude of experimentally observed disturbance waves are strongly decayed by nonlinear effect.
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  • Toru SAWAI, Mitsushi OHMASA, Noriyasu HIROKAWA, Masuo KAJI
    Article type: Original Article
    2009Volume 9Issue 4 Pages 338-344
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    To investigate the effect of the entry configuration of gas flow on the mechanism of flooding and to propose the prediction model of flooding, experiments of counter-current air-water two-phase flow are conducted. Two different types of inlet devices are used in the present study: “Bottom Entry” and “Nozzle Entry”. The effect of liquid viscosity on flooding is also investigated by using three kinds of temperatures of fluids 17°C, 30°C, and 47°C. Simultaneous measurements of the pressure drop and the spatio-temporal gas-liquid interfacial structure are conducted to detect the change in flow characteristics at the onset of flooding. The results obtained are as follows. The mechanism of flooding greatly depends on the entry configuration of gas flow. In the “Bottom Entry” device, large liquid lump formed near the liquid outlet are closely related to the onset of flooding. At flooding, the pressure gradient jumps up and a sudden and sufficient increase in the liquid holdup is observed. In the “Nozzle Entry” device, there are no appreciable changes in the pressure gradient and the gas-liquid interfacial stucture. The flow model to predict the onset of flooding is presented by considering the steady state momentum equations and the liquid lump formation at the bottom of the tube. It is found that the model can predict the flooding gas velocity for both inlet devices.
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  • Yoshiaki UEDA, Sho YOKOYAMA, Toshio ISHII, Manabu IGUCHI
    Article type: Original Article
    2009Volume 9Issue 4 Pages 345-350
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    The purpose of this paper is to numerically investigate behavior of a rising bubble near an orifice set in a stagnant water-filled vertical pipe. The orifice is selected in two kinds of the contraction ratio β between the pipe diameter D and the orifice one D0:β=D0⁄D=0.4 and 0.7. The rising bubble, of the area equivalent diameter being dB=0.5 D, whose wake-width is wider than D moves upward through the orifice of β = 0.7 with being elongated and contracted, whereas a small bubble of dB = 0.25 D = 0.36 D0 totally behaves like a bubbly flow even inside the orifice (i.e., the bubble rises with a zigzag motion). At the contraction ratio of β = 0.4, two kinds of patterns are successfully observed for a bubble captured at the orifice; (i) the bubble is settled behind the orifice under a hydrophilic condition, (ii) the bubble is settled inside the orifice under a hydrophobic condition. The physical discussion is addressed on the force balance of the meniscus.
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  • Keiji MURATA, Keisuke OKAMOTO, Koichi ARAGA
    Article type: Original Article
    2009Volume 9Issue 4 Pages 351-356
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    This paper presents an experimental investigation on forced convective boiling of a refrigerant HCFC123 in a mini-tube. The inner diameters of the test tubes, D are 0.51mm and 0.30mm. First, two-phase frictional pressure drops were measured in adiabatic conditions, and compared with the correlations for conventional tubes. The frictional pressure drop data were lower than the correlation for conventional tubes. However, the data were in accord with those for conventional tubes qualitatively, and correlated in the form ΦL2-1⁄Xtt. Next, heat transfer coefficients were measured in conditions of constant heat flux, and compared with those for conventional tubes. The heat transfer characteristics for min-tubes were different from those for conventional tubes, and so complicated. The heat transfer coefficients for D=0.51mm increased with heat flux, but were almost independent of mass flux. Although the heat transfer coefficients were higher than those for a conventional tube (D=10.3mm) in low quality region, they decreased with quality. The heat transfer coefficients for D=0.30mm were higher than those for D=0.51mm, and almost independent of both mass flux and heat flux.
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  • Koichi ARAGA, Shinnichi ITOGAWA, Yosuke NAKAMIZO, Keiji MURATA
    Article type: Original Article
    2009Volume 9Issue 4 Pages 357-362
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    It is known that small quantities of surfactant additives can greatly reduce the friction factors during the flow of a heat transfer medium. The friction factors are reduced because the generation of turbulent vortices is suppressed by the formation of rod-like micelles, and the flow remains laminar in the high Reynolds number range. However, the values of heat transfer coefficients decrease during flow laminarization; as a result, heat exchangers with a larger heat transfer area will be required. The research objective is to study the heat transfer enhancement effect of air injection. This paper presents an experimental investigation of the heat transfer and flow characteristics of an air-surfactant solution two-phase flow through a vertical tube. In the experiment, air was injected through a porous metal or a T-joint. The experimental results are as follows. In each air-inlet condition, heat transfer coefficients were enhanced drastically with the injection of air into a drag-reducing surfactant solution flow. In the case of air injection using porous metal, the flow patterns were almost bubbly flow at all flow rates. With regard to the enhancement rate of heat transfer coefficients, air injection through porous metal was more effective than that through the T-joint. This result shows that the apparent concentration of the surfactant solution in the bubbly flow was considerably less than that in any other flow patterns, because the surfactant molecules were concentrated at the bubble-water interface.
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  • Akira KATO, Tin Aung MOE, Satoshi KOHMURA
    Article type: Original Article
    2009Volume 9Issue 4 Pages 369-375
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    We have investigated a method to evaluate fatigue damage of mild steels without contact using laser. In high cycle fatigue of mild steels, we used a laser spot beam illuminating the fatigue damaged point of a specimen surface and observed diffusion pattern change of the reflected light from the specimen surface due to surface change by slipband in the previous work. This method was a point method observing at a point where spot beam is illuminating. In this paper, we tried to detect fatigue damaged area in the full field of the observing area with a CCD camera and evaluate fatigue damage using an optical setup with a laser slit beam. The results showed that there is a possibility of detecting fatigue damaged area and also evaluating fatigue damage by this optical setup. Full-field visualization and evaluation of fatigue damage is possible by scanning the slit beam on the specimen surface and observing reflected light pattern of the slit beam. There is also a possibility to predict a position where final fracture occurs based on the distribution of evaluated fatigue damage inside the fatigue area.
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  • Hironori IMAI, Tomoyuki OKADA, Nobuyoshi FUJIMATSU, Satoru YONEYAMA
    Article type: Original Article
    2009Volume 9Issue 4 Pages 376-381
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    An iterative method for determining three-dimensional coordinates of a planar object surface from a pair of images obtained by a stereovision is proposed. The three-dimensional coordinates of an object surface are obtained from the pair of the image coordinates of the corresponding points. Then, the camera parameters are refined using the coordinates of the object surface. Repeating this procedure, the accurate three-dimensional coordinates of the planar object surface are obtained. The effectiveness of the proposed method is validated by evaluating the three-dimensional coordinates of a planar board. In addition, the proposed method is applied to the measurement of the crack tip displacement fields and the subsequent stress intensity factors evaluation. Results show that the accu-racy for determining three-dimensional coordinates of a planar object is improved by the proposed method.
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  • Koichi HAYASHI, Ryuji TAKAGI, Takatomo YAMADA, Yasushi IDO
    Article type: Original Article
    2009Volume 9Issue 4 Pages 382-387
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    Magnetic functional fluids contain many magnetic particles. When the magnetic functional fluids including both micrometer size magnetic particles and nanometer size magnetic particles are used for the damper, the damping properties are affected by mixture ratio of them. The magnetic functional fluids including much micrometer size magnetic particles has large damping force. However the micrometer size magnetic particles sink immediately. Therefore, in this study, damping properties of a damper using magnetic functional fluids including both micrometer size magnetic particles and nanometer size magnetic particles are investigated experimentally. The magnetic functional fluids include thickener to prevent the magnetic particles from sinking. It is shown that the damping force, the absorption energy and the response of damping force are affected by the composition of the magnetic functional fluids.
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  • Takenobu SAKAI, Soichiro UENO, Koichi YAMADA, Satoshi SOMIYA
    Article type: Original Article
    2009Volume 9Issue 4 Pages 388-394
    Published: 2009
    Released on J-STAGE: June 25, 2010
    JOURNAL FREE ACCESS
    It is considered that there are two factors for polymer crystallization. One is crystallinity which is calculated by ratio of crystal and amorphous part, the other is crystalline state which represents interior morphology. Thus, adjustment of crystallinity and crystalline state was performed. As a result, crystal of POM is made up with spherulite. At first, crystal nucleation was observed. After then, crystalline growth occur radially from crystalline nucleus. It was understood to be able to make the sample with a different spherulite size by non-isothermal crystallization which means changing of cooling rate from melting condition. The other hand, crystallinity was increased with holding time remaining the shape of spherulite by isothermal crystallization. On each material, Arrhenius type of time-temperature superposition principle was confirmed on creep test. Creep behavior was suppressed with crystallinity by comparison between creep curves. However, it was confirmed that the shape of master curves are different between materials with different crystal grain size, because response of creep deformation to time passage is not same. Therefore, it was found that Grand master curve was obtained under the terms of same crystalline state, and it was able to estimate long term creep behavior on materials of arbitrary time, temperature and crystallinity.
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