The solution of a number of practical problems, in particular, the contactless investigation of shock processes, requires the multichannel extraction of information from different points of the object being measured. The operating principle of multichannel interferometers, like that of single-channel interferometers, is based on the use of the Doppler effect, i.e., on measuring the Doppler frequency, which is detected by superimposing two waves shifted in frequency with respect to one another. We can divide multichannel interferometers into two groups depending on their construction: those with normally incident optical signals in the reference and measuring arms of the interferometer, and those in which the optical signals are incident at different angles [I]. The incidence of optical signals at different angles is due to the change in the frequency modulation index, and enables the measurement limits to be changed. A multichannel vibratlon-resistant measuring system belonging to the first group is shown in Fig. la. Radiation from the source 1 is converted into n parallel beams by means of the splitter I. The first reference beam is directed via the splitter II onto the reflecting surface of the vibrator support i0, and the remaining measuring beams are directed via electrooptical transducers consisting of quarter-wave plates 2 and 5, lithium niobate crystals 3, fed from a shaper 4 and the beam splitting device II onto the reflecting surface II of the object being measured. The optical signals reflected from i0 and ii are combined in space using the beam splittee II and are applied to the photoreceiver 13 via the polarizer 12.
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