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US3719906A Expired / Lapsed US ⏱️ 0.0 years remaining

Dispersive delay lines operating in the shear mode

Assignee: Thales SA
•
Filing: 1970-11-12
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Granted: 1973-03-06
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Expires: 1990-11-12
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Abstract

Abstract A wave transmission medium has a pair of wave coupling arrays (41, 42) coupled thereto, each including a plurality of rectilinear, co-planar parallel excitation elements, spaced from each other by a predetermined distance a; the wave reception array being located on the transmission medium with respect to the wave transmission array to receive waves at an angle Alpha transmitted into said medium, when a transversely polarized wave is applied to the transmission array, with a direction of oscillations parallel to the co-planar excitation elements; the angle Alpha having a predetermined relation to the wavelength and propagation velocity of waves within the medium.

Inventors

  • 👤 P Tournois

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-25 18:50
CPC Classifications
H; H03; H03H; H03H9/00; H03H9/15; H03H9/17; G; G02; G02B; G02B27/00; G02B27/42; G02B27/4233; H04; H04R; H04R17/00; H04R17/04; H04R17/08

Claims Analysis

Total Claims: 23
Claim 1
Independent Claim 322 words
Dispersive delay line with an approximately linear time delay variation versus frequency over a large relative bandwidth and operation based on surface wave diffraction by periodic gratings, said line comprising : a propagation medium body 2 with parallel, plane faces 31,32 and a thickness d larger than the wavelength lambda of therein radiated elastic wave ; input and output elastic wave coupling means 1 ; 11,12, . . . input and output elastic wave type transducers 41, 42 located between said coupling means and at least one face of said medium and each comprising a plurality of rectilinear, co-planar, parallel grating elements presenting a periodic discontinuity in a corrugated pattern with an uniform corrugation pitch a forming a diffraction grating, one said grating element upon excitation generating an input surface wave, or ''''lateral wave,'''' and forming a bulk wave transducer 41 to propagate an elastic wave governed by a phase condition defined by the relationship phi n (2 pi f)/(C2) mna wherein n is the order number of the grating elements , C2 is the radiated wave propagation velocity in the said medium 2 , f is the received wave frequency and m is a parameter number, greater than one, depending on applied wave angle of incidence (sin Alpha 1) and the wave velocity ratio (C2/C1) and chosen in accordance with the desired time delay ( Delta t) and the wave frequency variations, said input diffraction grating 41 radiating a shear-bulk wave having a direction of oscillation parallel to said grating elements and an angle of emergence Alpha 2 in said medium dependent on wave frequency in accordance with the relation sin Alpha 2 m - p (C2)/(af) wherein p is a positive integer representing the diffraction order of the radiated wave energy, said wave energy being propagated through the medium irradiating the bulk-surface wave transducer output grating 42 at the same angle of incidence as the emergence angle Alpha 2 .
Claim 2
Dependent Claim 322 words
Dispersive delay line with an approximately linear time delay variation versus frequency over a large relative bandwidth and operation based on surface wave diffraction by periodic gratings, said line comprising : a propagation medium body 2 with parallel, plane faces 31,32 and a thickness d larger than the wavelength lambda of therein radiated elastic wave ; input and output elastic wave coupling means 1 ; 11,12, . . . input and output elastic wave type transducers 41, 42 located between said coupling means and at least one face of said medium and each comprising a plurality of rectilinear, co-planar, parallel grating elements presenting a periodic discontinuity in a corrugated pattern with an uniform corrugation pitch a forming a diffraction grating, one said grating element upon excitation generating an input surface wave, or ''''lateral wave,'''' and forming a bulk wave transducer 41 to propagate an elastic wave governed by a phase condition defined by the relationship phi n (2 pi f)/(C2) mna wherein n is the order number of the grating elements , C2 is the radiated wave propagation velocity in the said medium 2 , f is the received wave frequency and m is a parameter number, greater than one, depending on applied wave angle of incidence (sin Alpha 1) and the wave velocity ratio (C2/C1) and chosen in accordance with the desired time delay ( Delta t) and the wave frequency variations, said input diffraction grating 41 radiating a shear-bulk wave having a direction of oscillation parallel to said grating elements and an angle of emergence Alpha 2 in said medium dependent on wave frequency in accordance with the relation sin Alpha 2 m - p (C2)/(af) wherein p is a positive integer representing the diffraction order of the radiated wave energy, said wave energy being propagated through the medium irradiating the bulk-surface wave transducer output grating 42 at the same angle of incidence as the emergence angle Alpha 2 .
Claim 3
Dependent Claim 322 words
Dispersive delay line with an approximately linear time delay variation versus frequency over a large relative bandwidth and operation based on surface wave diffraction by periodic gratings, said line comprising : a propagation medium body 2 with parallel, plane faces 31,32 and a thickness d larger than the wavelength lambda of therein radiated elastic wave ; input and output elastic wave coupling means 1 ; 11,12, . . . input and output elastic wave type transducers 41, 42 located between said coupling means and at least one face of said medium and each comprising a plurality of rectilinear, coplanar, parallel grating elements presenting a periodic discontinuity in a corrugated pattern with an uniform corrugation pitch a forming a diffraction grating, one said grating element upon excitation generating an input surface wave, or ''''lateral wave,'''' and forming a bulk wave transducer 41 to propagate an elastic wave governed by a phase condition defined by the relationship phi n (2 pi f)/(C2) mna wherein n is the order number of the grating elements , C2 is the radiated wave propagation velocity in the said medium 2 , f is the received wave frequency and m is a parameter number, greater than one, depending on applied wave angle of incidence (sin Alpha 1) and the wave velocity ratio (C2/C1) and chosen in accordance with the desired time delay ( Delta t) and the wave frequency variations, said input diffraction grating 41 radiating a shear-bulk wave having a direction of oscillation parallel to said grating elements and an angle of emergence Alpha 2 in said medium dependent on wave frequency in accordance with the relation sin Alpha 2 m - p (C2)/(af) wherein p is a positive integer representing the diffraction order of the radiated wave energy, said wave energy being propagated through the medium irradiating the bulk-surface wave transducer output grating 42 at the same angle of incidence as the emergence angle Alpha 2 .
Claim 4
Dependent Claim 322 words
Dispersive delay line with an approximately linear time delay variation versus frequency over a large relative bandwidth and operation based on surface wave diffraction by periodic gratings, said line comprising : a propagation medium body 2 with parallel, plane faces 31,32 and a thickness d larger than the wavelength lambda of therein radiated elastic wave ; input and output elastic wave coupling means 1 ; 11,12, . . . input and output elastic wave type transducers 41, 42 located between said coupling means and at least one face of said medium and each comprising a plurality of rectilinear, coplanar, parallel grating elements presenting a periodic discontinuity in a corrugated pattern with an uniform corrugation pitch a forming a diffraction grating, one said grating element upon excitation generating an input surface wave, or ''''lateral wave,'''' and forming a bulk wave transducer 41 to propagate an elastic wave governed by a phase condition defined by the relationship phi n (2 pi f)/(C2) mna wherein n is the order number of the grating elements , C2 is the radiated wave propagation velocity in the said medium 2 , f is the received wave frequency and m is a parameter number, greater than one, depending on applied wave angle of incidence (sin Alpha 1) and the wave velocity ratio (C2/C1) and chosen in accordance with the desired time delay ( Delta t) and the wave frequency variations, said input diffraction grating 41 radiating a shear-bulk wave having a direction of oscillation parallel to said grating elements and an angle of emergence Alpha 2 in said medium dependent on wave frequency in accordance with the relation sin Alpha 2 m - p (C2)/(af) wherein p is a positive integer representing the diffraction order of the radiated wave energy, said wave energy being propagated through the medium irradiating the bulk-surface wave transducer output grating 42 at the same angle of incidence as the emergence angle Alpha 2 .
Claim 5
Dependent Claim 47 words
Delay line according to claim 1, wherein said transmission medium 2 is of the type capable of transmitting an acoustic shear wave; and the direction of oscillation of the applied wave coincides with the direction of oscillation of the shear wave generated by said transmission array 41.
Claim 6
Dependent Claim 115 words
Delay line according to claim 2 including (FIG. 4) a pair of acoustic wave transducers 51, 52 arranged to excite, or receive, polarized waves in a direction of polarization parallel to the elements of the arrays; coupling prisms 11, 12 each having a face 110, 120 in contact with said medium 2 and another face 111, 121 in contact with a respective transducer; the faces of the prisms 110, 120 which are in contact with the medium 2 making an angle Alpha 1 which is defined by sin Alpha 1 m (C1/C2) wherein C1 is the propagation phase velocity of said wave in the prism and C2 is the propagation phase velocity in said medium.
Claim 7
Dependent Claim 22 words
Delay line according to claim 3, wherein said arrays are cut into the faces of the prisms in contact with said medium.
Claim 8
Dependent Claim 36 words
Delay line according to claim 4, wherein (FIG. 9) said prisms are severed portions 11, 12 of a single block 10 said block having said arrays cut therein transversely to the severence line severing said portion.
Claim 9
Dependent Claim 47 words
Delay line according to claim 2, wherein (FIG. 7) said medium 2 has a reflective surface; and said arrays are located with respect to each other such that shear waves propagated into the medium reflect at said surface in their course from one array to the other.
Claim 10
Dependent Claim 52 words
Delay line according to claim 2, wherein (FIG. 8) said medium is in form of a lamella formed with a first face, said arrays being applied to said first face; and said lamella Is formed with a second face, said second face being reflective to shear waves applied thereto by said arrays.
Claim 11
Dependent Claim 15 words
Delay line according to claim 7, wherein said first and said second faces are parallel.
Claim 12
Dependent Claim 30 words
Delay line according to claim 1, wherein (FIGS. 1, 4, 7, 11) said medium 2 has a pair of parallel faces, and said arrays are applied to said parallel faces.
Claim 13
Dependent Claim 47 words
Delay line according to claim 1, including (FIGS. 4, 7, 8, 10) at least one coupling prism covering an array, and an electro-acoustic transducer applied to said prism, said prism having a oblique face with respect to the contact face of the prism covering the respective array.
Claim 14
Dependent Claim 35 words
Delay line according to claim 10, including (FIG. 10) a second coupling prism covering the other array and having a reflecting face which is oblique with respect to the contact face of said second array.
Claim 15
Dependent Claim 124 words
Delay line according to claim 11, wherein (FIG. 10) said first prism has a transmitter-electro acoustic transducer applied thereto polarized to excite vibrations in said medium parallel to said elements of the array; and further has a receiver-electro acoustic transducer applied thereto, one each, to a respective face oblique with respect to the contact face of said prisms with a respective array; and said respective faces having said transducers applied thereto are inclined with respect to each other by an angle which is defined in accordance with the relationship sin Alpha 1 m (C1/C2) wherein C1 is the propagation phase velocity of said wave in the prism, C2 is the propagation phase velocity in said medium and m is a number greater than one.
Claim 16
Dependent Claim 147 words
Delay line according to claim 1, including (FIG. 11) an emitter piezo electric element; a receiver piezo electric element; said wave transmission and wave reception arrays being, respectively, cut into the respective piezo-electric elements, said piezo-electric elements being applied in contact with said medium 2; said arrays comprising rectilinear parallel electrodes equidistantly placed on faces of said piezo electric element; first delay means 61 applying to the respective electrodes of said emitter piezo element electrical potentials which are progressively delayed with respect to each other in accordance with the spacing of the electrodes; and second delay means 62 connected to the respective electrodes of the receiver piezo electric element, said second delay means transducing the potentials applied to the electrodes thereof which are progressively delayed with respect to each other in accordance with the spacing of the electrodes and delivering delayed signals at an output terminal (S).
Claim 17
Dependent Claim 36 words
Delay line according to claim 13, wherein said medium is a plate of piezo electric material and forms said elements, the piezo electric electrodes being directly applied to faces of said plate of piezo electric medium.
Claim 18
Dependent Claim 99 words
Delay line according to claim 1, wherein (FIG. 6) said medium is a lamella of transparent material having a pair of planar parallel faces; a pair of coupling prisms are provided applied to said plane faces of the lamella, and prisms covering said wave transmission and wave reception arrays, respectively; one of said prisms having an input face located to receive luminous radiant energy at an angle in excess of the critical angle of refraction; and said second prism having an output face located at an angle parallel to the angle of the input face of the first prism.
Claim 19
Dependent Claim 255 words
Method of delaying a wave signal, the delay being dependent on frequency of the signal comprising applying said signal to an array of parallel uniformly spaced grating elements on a medium capable of transmitting shear waves upon application of waves to said array; and detecting said shear waves in said medium by a similar array applied thereto; the step of applying said signal comprising the step of generating a polarized wave of said signal having a direction of polarization parallel to the elements of the arrays governed by the phase relationship phi n (2 pi f/C2) mna wherein n is the order number of the grating elements, C2 is the radiated wave propagation velocity in the said medium 2, f is the received wave frequency and m is a parameter number, greater than one, depending on applied wave angle of incidence (sin Alpha 1) and the wave velocity ratio (C2/C1) and chosen in accordance with the desired time delay ( Delta t) and the wave frequency variations; the step of introducing a shear bulk wave having a direction of oscillation parallel to said grating elements and an angle of emergence Alpha 2 in said medium dependent on wave frequency in accordance with the relation sin Alpha 2 m - p (C2/af) wherein p is a positive integer representing the diffraction order of the radiated wave energy, to propagate said wave energy through the medium; and the step of detecting said shear wave comprising the step of detecting shear waves propagated under an angle Alpha 2.
Claim 20
Dependent Claim 255 words
Method of delaying a wave signal, the delay being dependent on frequency of the signal comprising applying said signal to an array of parallel uniformly spaced grating elements on a medium capable of transmitting shear waves upon application of waves to said array; and detecting said shear waves in said medium by a similar array applied thereto; the step of applying said signal comprising the step of generating a polarized wave of said signal having a direction of polarization parallel to the elements of the arrays governed by the phase relationship phi n (2 pi f/C2) mna wherein n is the order number of the grating elements, C2 is the radiated wave propagation velocity in the said medium 2, f is the received wave frequency and m is a parameter number, greater than one, depending on applied wave angle of incidence (sin Alpha 1) and the wave velocity ratio (C2/C1) and chosen in accordance with the desired time delay ( Delta t) and the wave frequency variations; the step of introducing a shear bulk wave having a direction of oscillation parallel to said grating elements and an angle of emergence Alpha 2 in said medium dependent on wave frequency in accordance with the relation sin Alpha 2 m - p (C2/af) wherein p is a positive integer representing the diffraction order of the radiated wave energy, to propagate said wave energy through the medium; and the step of detecting said shear wave comprising the step of detecting shear waves propagated under an angle Alpha 2.
Claim 21
Dependent Claim 13 words
Method according to claim 16, wherein said wave signal is an acoustic signal.
Claim 22
Dependent Claim 13 words
Method according to claim 16, wherein said wave signal is a radiation signal.
Claim 23
Dependent Claim 14 words
Method according to claim 18, wherein said wave signal is a luminous radiation signal.

References Cited (Backward Citations)

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USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1976-03-05 1976-09-04 1977-03-06 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1980-03-05 1980-09-04 1981-03-06 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1984-03-05 1984-09-04 1985-03-06 $7700.00 Window Closed / Lapsed

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