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Method and system for determining the angle of deviation of an axis

机译:确定轴线偏离角的方法和系统

摘要

1,070,655. Axis direction determination. BOLKOW G.m.b.H. Sept. 25, 1964 [Sept. 25, 1963], No. 39219/64. Heading H4D. The angle of deviation of an axis Z, Fig. 1, with respect to the direction of a celestial body 33, is determined, by forming an image 31 of the body on the screen of a television camera tube by means of a lens 30 having a field of view of 180 degrees, and by scanning the screen by means of two groups of ellipses, of which the major axes are perpendicular in respect of one another, and the minor axes, starting from a value of zero, are increased in accordance with a circular sinusoidal function up to the value of the major axis, the interval of time between the moment when a minor axis of an ellipse starts from a value of zero, and the moment when a scanning ellipse of the same group passes the image, being a direct measure for the magnitude of an angle of deviation # or #. It is shown in the Specification that the equation in the X, Y plane of the image 31 of a body 33 lying in a plane containing the X axis and at an angle # with the Z, X plane is the ellipse where 1/m is the focal length of lens 30, and it is likewise shown that the equation in the X, Y plane of the image 31 of a body 33 lying in a plane containing the Y axis and at an angle # with YZ plane is the ellipse Thus be determining the minor axis of the ellipse which passes through the image 31, the angle # or # may be directly determined. Referring to Fig. 3, lens (4) focusses the image (2) of the celestial body on the screen (3) of the television camera tube (1). The scanning spot of the camera tube is deflected by X and Y deflector plates, having sinusoidal deflecting voltages applied thereto from generator (6), that applied to the Y plates being phase shifted by means (8) with respect to that applied to the X plates. As such voltages would merely cause the spot to describe a circle, the deflection voltages are amplitude modulated in modulation stages (7) and (9). The modulation waveform consists of half sine waves alternating with rectangular pulses having the same amplitude and width, the sine waves being produced by generator (11) and the rectangular pulses by multivibrator (12). The modulation waveform applied to modulation stages (7) in 180 degrees out of phase with that applied to modulation stage (9) such that when the X plates are being energized with a deflection voltage of constant amplitude, the Y plates being energized with a deflection voltage whose amplitude varies in a sinusoidal manner, and vice versa. The result is that the screen is scanned with a first series of ellipses, starting as a line along say the X axis, and broadening out from ellipse to ellipse to finally give a circle, and then narrowing down again to the straight line. This is then repeated along the Y axis. Each series of ellipses thus scans the image twice and produces two output signals from the camera tube. Only the first sig. nal however is used. To determine the minor axis of the ellipse which passes through the image (13) a bi-stable multivibrator (16) is used, which is triggered on a synchronism with the start of the series of ellipses, and is triggered off by the first output signal from the camera tube, to give a pulse having a width indicating the minor axis. This width is converted to a pulse height by means of integrator (17) and differentiator (18). To determine whether the pulse height represents the angle # or the angle #, the pulse passes to gates (19) and (20), which are opened alternately in corresponding synchronism with the changeover of the alignment of the major axes of the ellipse series. To determine on which side of the X or Y axis the image lies, the outputs of gates (19) and (20) are fed to gate pairs (21/22) and (23/24). The first pair are alternately opened by the output of generator (6) such that a pulse represented by its height will pass through gate (21) if it is on the positive side of the X axis and through gate (22) if it is on the negative side of the X axis. Pulses represent + # and - # likewise come from gates (23) and (24) respectively. Generator (6) is synchronized at frequency f/400 by a pulse train at that frequency from trigger (5) via pulse divider (10) and multivibrators (12) and (16) are triggered by pulses f at frequency --- from trigger (5), via pulse 200 divider (10). If the field of view of the lens is less than 180 degrees the minor axis of the ellipse increases to a value proportionally less than the major axis.
机译:1,070,655。轴方向确定。 BOLKOW G.m.b.H. 1964年9月25日[9月[1963年5月25日],编号39219/64。标题H4D。图1的Z轴相对于天体33的方向的偏角是通过借助于具有以下特征的透镜30在电视摄象机的管的屏幕上形成人体的图像31来确定的。视场为180度,并通过两组椭圆扫描屏幕,椭圆的长轴相对于彼此垂直,短轴从零开始增加通过一个正弦函数直到主轴值,椭圆的短轴从零值开始到同一组的扫描椭圆通过图像之间的时间间隔,是偏差角度#或#的大小的直接量度。在说明书中示出,位于包含X轴并且与Z,X平面成角度#的平面中的物体33的图像31的X,Y平面中的方程是椭圆,其中1 / m是同样表明,位于包含Y轴且与YZ平面成角度#的物体33的图像31的X,Y平面中的方程是椭圆,因此在确定穿过图像31的椭圆的短轴时,可以直接确定角度#或#。参照图3,透镜(4)将天体的图像(2)聚焦在电视摄象管(1)的屏幕(3)上。显像管的扫描光斑被X和Y偏转板偏转,X和Y偏转板从发生器(6)施加正弦偏转电压,施加到Y板上的电压通过装置(8)相对于施加到X的相移。盘子。由于这样的电压将仅使斑点描述一个圆,因此在调制级(7)和(9)中对偏转电压进行幅度调制。调制波形由半正弦波与具有相同幅度和宽度的矩形脉冲交替组成,正弦波由发生器(11)产生,矩形脉冲由多谐振荡器(12)产生。施加到调制级(7)的调制波形与施加到调制级(9)的调制波形异相180度,这样,当X板以恒定幅度的偏转电压通电时,Y板以偏转电压通电振幅以正弦形式变化的电压,反之亦然。结果是用第一批椭圆形扫描屏幕,从沿着X轴的一条线开始,从椭圆形变宽到椭圆形,最后给出一个圆,然后再缩小到直线。然后沿着Y轴重复此操作。因此,每个椭圆系列将扫描图像两次,并从摄像管产生两个输出信号。只有第一个信号。但是使用了nal。为了确定穿过图像(13)的椭圆的短轴,使用了双稳态多谐振荡器(16),该振荡器与一系列椭圆的开始同步触发,并由第一个输出触发来自摄象机筒的信号,以给出一个具有指示短轴的宽度的脉冲。该宽度通过积分器(17)和微分器(18)转换为脉冲高度。为了确定脉冲高度代表角度#还是角度#,脉冲传递至门(19)和(20),门与椭圆系列的主轴排列的转换相应同步地交替打开。为了确定图像位于X轴或Y轴的哪一侧,门(19)和(20)的输出被馈送到门对(21/22)和(23/24)。第一组通过发生器(6)的输出交替打开,以使其高度表示的脉冲在X轴的正侧通过门(21),在打开时通过门(22)。 X轴的负侧。代表+#和-#的脉冲分别分别来自门(23)和(24)。发生器(6)通过脉冲分配器(10)从触发器(5)以该频率在脉冲f / 400处以脉冲频率进行同步,并且多谐振荡器(12)和(16)由脉冲f以触发频率---触发(5)通过脉冲200除法器(10)。如果镜片的视场小于180度,则椭圆的短轴会增加到与长轴成比例的值。

著录项

  • 公开/公告号GB1070655A

    专利类型

  • 公开/公告日1967-06-01

    原文格式PDF

  • 申请/专利权人 BOELKOW GMBH;

    申请/专利号GB19640039219

  • 发明设计人

    申请日1964-09-25

  • 分类号F41G7/34;G01S3/782;G01S3/786;

  • 国家 GB

  • 入库时间 2022-08-23 13:54:27

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