Patent GB-988102-A (GB)
Title: Improvements in or relating to wave-energy delay cells
Inventor: MORTLEY WILFRED SINDEN
IPC: H03H9/40
Filed: 1962-08-03
Abstract: 988,102. Electromechanical delay lines. MARCONI CO. Ltd. May 20, 1963 [Aug. 3, 1962], No. 29851/62. Heading H3U. A frequency-dispersive delay cell includes a transmissive or reflective grating, the grating having graded spacings chosen so as to subject waves of different frequencies to different delays. As shown (Fig. 1), the cell comprises a slab 1 of fused quartz having input and outputpiezo-electric transducers 2, 3 on two mutually perpendicular faces, and a reflective grating 4 on an inclined face. The geometry of the body 1 and the spacing of the lines in the grating are such that each different part of the grating will selectively reflect in the direction of the output transducer 3 a different frequency in a swept range of frequencies applied to the input, whereby each frequency suffers a different delay. Thus a long swept train of frequencies applied to the input may be arranged to generate a short output pulse of frequencies if the grating is such that the delay decreases from a maximum for the frequencies at the beginning of the swept train to a minimum for the frequencies at the end of the train. To this end, the spacings, which may be of the order of twice one wavelength, increase, preferably linearly, from one end of the grating to the other. When used in reverse, the grating transforms a short pulse into a long swept train. The grating may be cut into the face 1D of the transmission body and is backed by absorptive material, e.g. solder, which surrounds the whole body and serves to dissipative unwanted signal energy. The greater part of the latter consists of specular reflections from the grating incident mainly on the facet 1B. This facet may be inclined at an angle of 30 degrees to the major faces of the body 1 whereby the unwanted energy is caused to suffer multiple reflection between these faces. The intensity of the unwanted reflections may be reduced by using transducers having tapered characteristics, whereby the point of greatest wave amplitude moves along the transducer as the frequency sweeps and only that part of the grating which reflects a useful signal is strongly illuminated. In place of long transducers extending over the appropriate facets, linear arrays of elemental transducers may be used. Such transducers are so shaped that the dividing lines between adjacent elements are not at right-angles to the longitudinal axis of the array. The modified delay cell of Fig. 5 uses a transmissive grating 44 of the form indicated in Fig. 6. The output transducer 3 is positioned behind the grating and energy passes to the transducer through the flat faces 44A which constitute the lines of the grating. Unwanted energy is reflected towards an inclined facet F. In the modification shown in Fig. 7, the transmissive grating 44 is illuminated by two input transducers 2A, 2B which are identical except for the fact that opposite directions of sweep must be applied in order to produce an output pulse from the transducer 3. In a further modification of the invention the functions of the transmitting body, the grating and the transducers are combined by using a body of piezo-electric quartz or barium titanate provided with input and output electrodes in the form of interdigitated combs 1K1, 1K2, Fig. 10, having graded spacings between the teeth. The combs are made from deposited gold and are provided with terminals 2K1, 2K2 in the form of silver spots. Each electrode array is arranged on the inclined surfaces of a piezo-electric quartz slab having a section of isoceles-triangular form. The third facet is covered with dissipative material. If the X-axis of the quartz is arranged to coincide with the direction of propagation, signals applied to the comb electrodes will produce shear stresses in the quartz and a transverse wave will be propagated. Each electrode array is arranged to provide half the total dispersion. The Specification also refers to the use of both transverse and longitudinal waves, the use of liquid and gaseous delay cells and to curved gratings. A magnetostrictive transducer using a body of ferromagnetic material bearing a deposited zig-zag conductor is briefly described.