Aeronautical and Space Sciences Japan
Online ISSN : 2424-1369
Print ISSN : 0021-4663
ISSN-L : 0021-4663
Volume 35, Issue 403
Displaying 1-6 of 6 articles from this issue
  • Shuji NISHI
    1987 Volume 35 Issue 403 Pages 363-369
    Published: August 05, 1987
    Released on J-STAGE: December 16, 2010
    JOURNAL FREE ACCESS
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  • Yoshio TAKAKSA
    1987 Volume 35 Issue 403 Pages 370-378
    Published: August 05, 1987
    Released on J-STAGE: December 16, 2010
    JOURNAL FREE ACCESS
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  • Yoshiaki HAYAKAWA, Hitoshi NIBE
    1987 Volume 35 Issue 403 Pages 379-388
    Published: August 05, 1987
    Released on J-STAGE: December 16, 2010
    JOURNAL FREE ACCESS
    Uncertainty in a gyro design means unpredicted problems in design phase, and this will introduce uncompensated errors which must be charged to the gyro. Uncompensated errors in gyros are as follows. (1) Drift instability, (2) Scale factor instability, (3) Temperature coefficient of drift and its instability. As an uncertainty or instability of gyro output is related to not only a design but also manufacturing as causing a change in the location and a randomly substance of adhesive, etc, it is difficult to make clear the level in design phase. However, it is important to find out the principles governing parameters for instability or uncertainty of gyro output. Then, a Day-to-Day stability and a Temperature Coefficient of G-insensitive Drift for TDGs was measured, and furthermore, In-phase spring rate, Quadrature spring rate and offset angle which consist of G-insensitive drift of TDG was measured. As a result of these testings, it was found out that the governing parameter for instability or uncertainty of TDG G-insensitive drift was mainly dependent on offset angle variation. This conclusion will be effective to introduce more accurate TDG in design and fabrication.
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  • Makoto KOBAYAKAWA, Masahiro NAKAO
    1987 Volume 35 Issue 403 Pages 389-398
    Published: August 05, 1987
    Released on J-STAGE: December 16, 2010
    JOURNAL FREE ACCESS
    In order to investigate the flow field around the ATP through numerical methods for its optimal design, 3D-Euler equations are most prominent. The flow field around counter rotating propellers in advancing 0.8 Mach is obtained. Two spaces including front and rear blades are solved separately. The interaction between both blades are taken into the calculation by the connecting surfaces. The noniterative implicit ADI scheme is used in order to solve Euler equations. The periodic steady and averaged steady solutions are obtained. The latter is simplified by averaging the variables at the connecting surface. This shortens the calculation time to one-third comparing with the periodic steady analysis which simulates the relative motion of the blades exactly. Numerical calculations are performed for two counter rotating ATP's with SR-1 and SR-3 blades. Both results show that they are similar with each other, and the propeller efficiencies increase comparing with single rotating ATP with same blades.
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  • Kenji INOUE, Takashi NAKAMURA
    1987 Volume 35 Issue 403 Pages 399-400
    Published: August 05, 1987
    Released on J-STAGE: December 16, 2010
    JOURNAL FREE ACCESS
    Two things to be added to a previously published paper on the calculation of the transonic potential flow through a two-dimensional cascade are stated. The first is the procedure of calculation to obtain the solution in which a given point on a blade is a stagnation point without giving the downstream condition. The second is the relation between the force acting on a blade, the distribution of pressure on its surface, the circulation around it and the up- and downstream conditions.
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  • Takaaki HASHIMOTO
    1987 Volume 35 Issue 403 Pages 401-404
    Published: August 05, 1987
    Released on J-STAGE: December 16, 2010
    JOURNAL FREE ACCESS
    A design method of the cascade for a shock-in-rotor supersonic axial-flow compressor is presented. The inlet flow is uniform and satisfies simplified radial equilibrium. The flow just before the normal shock is uniform and satisfies simplified radial equilibrium. The supersonic portion between the inlet and the normal shock is designed by using the method of weak wave. In the subsonic portion the flow is quasi-axisymmetric. The shape of mean streamline is assumed to be circular arc. The passage walls are composed of circular arcs. A two-dimensional supersonic cascade which is designed by the method in this report includes the three-dimensional effect by taking into account radial equilibrium conditions.
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