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New projection system for television images

机译:新的电视影像投影系统

摘要

909,401. Television; light modulating. GENERAL ELECTRIC CO. Jan. 5, 1959 [Jan. 13, 1958], No. 339/59. Class 40 (3). In a television receiving system in which deformations produced in a deformable medium by electrostatic charges varying in accordance with the image signals are employed to modulate light from a local source which is then projected on to a viewing screen the deformations produced during each field scan are erased, coincidently with, or just prior to, the setting up of deformations in the next field scan by scanning the medium with an unmodulated electron beam the energy of which, relative to the average potential of the medium for the desired amplitudes of deformation, is equal to that value at which the characteristic relating beam energy and secondary emission ratio for the medium passes through unity for the second time. This point, termed the " second secondary emission cross-over potential " is shown at 49 (Fig. 2) and by arranging the potential of the unmodulated erasing electron beam 13 (Fig. 1) which scans the deformable medium 15 to be less than the required potential of the medium relative to the electrode 19, e.g. - 500 V. medium to electrode and -1900 (from curve) electron gun 11 to medium, giving - 2400 gun to electrode 19, the potential of the medium is brought to - 500 V. (undeformed value) irrespective of its initial condition since a surplus or deficiency of electrons on the medium is neutralized by the change in secondary emission ratio above and below unity due to the effective change in beam energy. With this manner of operation the resistance of the medium 15 may be high enough for the deformation to persist for a complete field period with a consequent improvement in the light efficiency of the system. Molten paraffin or white beeswax or a gelatin are suitable materials. In the embodiment of Fig. 1 the image signals are supplied to the electrode 19 from source 27 so that each point on the medium, after the passage of the beam 13, is left with a charge, relative to electrode 19, and therefore with a deformation appropriate to the image signals appertaining to that point. In a second embodiment (Figs. 3 and 4) the image deformations are produced by a modulated " point-focused " beam 57 and erasure produced by an unmodulated " line-focused," beam 53 which scans the medium 15 in the frame direction a short distance ahead of beam 53. In both embodiments the medium 15 is included in a conventional optical system 29 . . . 39 which projects the image on to a viewing screen 41. Instead of utilizing light transmitted through the deformable medium the optical system may be modified to utilize light reflected from the surface of the medium.
机译:909,401。电视;光调制。通用电气公司,1959年1月5日[Jan. [1958年13月13日],第339/59号。 40级(3)。在电视接收系统中,通过根据图像信号变化的静电荷在可变形介质中产生的变形被用来调制来自本地光源的光,然后将其投射到显示屏上,消除了每次场扫描期间产生的变形。通过与未调制电子束扫描介质,在下一场扫描中恰好相吻合,或者恰好在此之前,通过未调制电子束扫描介质,该能量的能量相对于介质在期望变形幅度上的平均电势等于等于该值,介质的束能和二次发射比的特性曲线第二次通过。这一点被称为“第二二次发射交叉电势”,显示在49(图2),并通过布置未调制擦除电子束13(图1)的电势来扫描可变形介质15,使其小于相对于电极19的介质所需的电势,例如-500 V.介质到电极,-1900(从曲线)电子枪11到介质,-2400电子枪到电极19,介质的电势达到-500 V.(未变形值),而与初始条件无关,因为由于电子束能量的有效变化,二次发射比的变化大于或小于1,可以抵消介质上电子的过剩或不足。通过这种操作方式,介质15的电阻可以足够高,以使得变形在整个场周期内持续存在,从而改善了系统的光效率。熔融的石蜡或白蜂蜡或明胶是合适的材料。在图1的实施例中,图像信号从源27被提供给电极19,使得在束13通过之后,介质上的每个点相对于电极19被留下电荷,并且因此被保留。适于该点图像信号的变形。在第二实施例中(图3和图4),图像变形是由调制的“点聚焦”光束57产生的,而擦除是由未调制的“线聚焦”光束53产生的,该光束在帧方向a上扫描介质15。在光束53之前较短的距离。在两个实施例中,介质15都包括在常规光学系统29中。 。 。如图39所示,其将图像投影到观察屏41上。代替利用通过可变形介质透射的光,可以修改光学系统以利用从介质表面反射的光。

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