| 摘要 |
993,072. Electric selective signalling. FERRANTI Ltd. March 11, 1964 [March 21, 1963], No. 11165/63. Heading G4H. Signals are derived representing the extent and sense of the movement of an object by laser means tuned to a predetermined frequency and having light sensitive means arranged to produce two signals, a mirror or mirrors at the other end attached to the moving object so as to reflect back part of the radiation from the laser means, movement causing amplitude modulation of the signals, the signals being representative of two optical paths of slightly different lengths from the laser means to the moving object and back so that the signals are in quadrature phase, the timed relationmovement being indicated by the timed relationship between the two signals. In Fig. 2 a worktable W of a machine tool carries two mirrors R1, R2 each co-operating with a laser L1, L2. The lasers are tuned to the same frequency and each has a photo-cell P1, P2. The mirrors are placed so that the difference in distance is one-eighth of the wavelength. As the work-table moves the signals from the two photo-cells are amplitude modulated sinusoidally and are phase displaced by a quarter wavelength. The cycles are counted at E. The counter may be controlled as in Specification 760,321 to count forwards or backwards according to the direction of movement as is indicated by the time relationship between the two signals. The quarter wavelength phase displacement may alternatively be produced by a compensating plate or by shifting the lasers, the mirrors R1, R2 being aligned. To avoid using two mirrors, a single mirror R3, Fig. 3, may be used, the two optical paths coinciding between mirror R3 and half-mirror 22. Mirror 21 reflects light reflected from half-mirror 22 to laser L1, one beam is delayed a quarter wavelength by plate C. To avoid interference between the two beams they are polarised at right-angles by transparent plates 23, 24. To avoid disparities due to changes in the parameters of the Lasers they may be arranged to share the same gas filling, the same excitation and the same resonator mirrors. In the form of Fig. 5 a single laser L3 is used on a time-sharing basis, the optical path to the mirror being short or long according as to whether delay device is energized. This is controlled by a generator 42 which provides a square-wave signal. The output of photo-cell P3 is switched to lead 44 or lead 45 by the generator 42 so that one lead receives signals relating to the short path and the other to the long path. The resultant signals (Fig. 6) are smoothed to obtain the two quadrature displaced signals. A double laser as shown in Fig. 4 may be combined with a timesharing arrangement as shown in Fig. 5 to produce four signals each displaced by 90 degrees from the next. The photo-cells may be placed at the other ends of the lasers but this is less convenient.
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