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    • 42. 发明专利
    • Hologram preparing method
    • HOLOGRAM制备方法
    • JPS60190818A
    • 1985-09-28
    • JP4682984
    • 1984-03-12
    • Mitsubishi Heavy Ind Ltd
    • MURATA MASAYOSHIKURODA MASAHIRO
    • G01B9/021G01H9/00G03H1/04
    • G01H9/002G01B9/021
    • PURPOSE:To enable to apply the method to the measurement of vibrations widely regardless of steady state vibration or non-steady state vibration, by simultaneously recording and reproducing two interference fringes representing the equal amplitude line of the vibration of a vibrating body and the direction and magnitude of the displacement of the vibration, i.e., the relative phases. CONSTITUTION:The two images of a body to be measured 124 are independently formed on first and second holographic photograph plates 112 and 303 by an image forming lens 300 and a beam splitter 301. The first reference light having a specified incident angle is used as reference light for the first holographic photograph plate 112. The second reference light, whose incident angles are different at the first shot and the second shot of double-pulse light, is used for the second holographic photograph plate 303. Thus the interference fringes representing the equal amplitude line of the vibration and the interference frings representing the direction and magnitude of the displacement of vibration, which show excellent contrast, can be obtained. Therefore the hologram, which can be widely applied not only in the steady state vibration of the body to be measured but also in the non-steady state vibration or exposure vibration, can be obtained.
    • 目的:通过同时记录和再现表示振动体的振动等振幅线的两个干涉条纹,以及方向和方向,能够广泛地将该方法应用于振动测量,而不管稳态振动或非稳态振动 振动位移的大小,即相对相位。 构成:被测体124的两个图像通过图像形成透镜300和分束器301独立地形成在第一和第二全息照相板112和303上。具有特定入射角的第一参考光被用作参考 第一全息照相板112的光。第二全息照相板303使用入射角在第一镜头不同的第二参考光和双脉冲光的第二镜头。因此,干涉条纹表示相等 可以获得振动的幅度线和表示振动位移的方向和幅度的干涉条纹,其显示出优异的对比度。 因此,可以获得不仅可以在被测体的稳态振动中,而且在非稳态振动或曝光振动中广泛应用的全息图。
    • 45. 发明专利
    • OSCILLATION MEASURING METHOD BY HOLOGRAPHY
    • JPS5897627A
    • 1983-06-10
    • JP19712081
    • 1981-12-08
    • MITSUBISHI HEAVY IND LTD
    • MURATA MASAYOSHIKURODA MASAHIRO
    • G01H9/00G03H1/04
    • PURPOSE:To measure various pieces of information which could not be obtained before securely by exciting a body to be tested bynthe percussion of a hammer and emitting pulse laser light before and after the generation of impulsive force, and thus obtaining a hologram. CONSTITUTION:When a switch 121 is turned off, a hammer 110 excites a bar 117 by percussion. The rotary movement start signal of the hammer 110 is detected by a pulse fall detector 124 and applied to a double pulse laser device 126 through a delay circuit 125. Double pulse light is split by a beam splitter 129 into two pieces of liminous flux; one piece of luminous flux is used as reference light to expose a photographic dry plate 135 through a plane mirror 130, concave lens 131, collimator lens 132, optical attenuator 133, and plane mirror 134. The other piece of luminous flux is used as object illumination light to illuminate the internal combustion engine crank case 100 to be tested through a concave lens 137. The photographic dry plate 135 is exposed to light when the 100 to be tested is at a still and 50musec after being excited together with the reference light.
    • 47. 发明专利
    • VIBRATION MEASURING METHOD BY PULSE LASER HOLOGRAPHY
    • JPS5444579A
    • 1979-04-09
    • JP11106077
    • 1977-09-14
    • MITSUBISHI HEAVY IND LTD
    • MURATA MASAYOSHIKURODA MASAHIRO
    • G01H9/00G03H1/04
    • PURPOSE:To obtain the modes and relative phases of vibration modes togeter with the information on amplitude distribution and perform accurate analysis of modes by reflecting two shots of illuminating rays of double pulse laser with a rotary reflecting means and projecting the same to the measuring object from different angles. CONSTITUTION:In making a hologram by projecting the pulse laser light emitted from a double pulse laser device 1 to the measuring object 11, a rotary reflecting mirror 23 is provided between a beam splitter 2 and the measuring object 11 and two shots of illuminating rays are reflected while this rotary reflecting mirror 23 rotates to project the rays to the measuring object from respectively differnt angles. Here, the measuring object 11 is vibrated by an exciter 16 and the first shot of the radiated there to in a vibration zero state while it is being monitored with an oscillo- scope 13. the angle of the illumination light is changed in various ways in the exposure of a photographic plate 8 so that interference fringes appear in the hologram reconstruction image. At the time of emitting the second shot of laser light, the rotary plane mirror 23 is made at a different angle and the laser light is raidated to the measuring object 11 in the maximum negative amplitude state and is exposed simultaneously to the photographic plate 8, whereby the hologram is obtained.