NO116769B - - Google Patents
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- Publication number
- NO116769B NO116769B NO162581A NO16258166A NO116769B NO 116769 B NO116769 B NO 116769B NO 162581 A NO162581 A NO 162581A NO 16258166 A NO16258166 A NO 16258166A NO 116769 B NO116769 B NO 116769B
- Authority
- NO
- Norway
- Prior art keywords
- sides
- output converter
- hit
- prism
- converter
- Prior art date
Links
- 238000002604 ultrasonography Methods 0.000 claims description 4
- 230000010355 oscillation Effects 0.000 description 3
- 239000005401 pressed glass Substances 0.000 description 3
- JRPBQTZRNDNNOP-UHFFFAOYSA-N barium titanate Chemical compound [Ba+2].[Ba+2].[O-][Ti]([O-])([O-])[O-] JRPBQTZRNDNNOP-UHFFFAOYSA-N 0.000 description 1
- 229910002113 barium titanate Inorganic materials 0.000 description 1
- 239000000463 material Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/30—Time-delay networks
- H03H9/36—Time-delay networks with non-adjustable delay time
Landscapes
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Description
Ultralydforsinkelsesanordning. Ultrasonic delay device.
Oppfinnelsen angår en ultralydforsinkelsesanordning med et prismeformet medium med hovedsakelig femkantet grunnflate og som dannes av to praktisk talt parallelle sider, en tredje side som står praktisk talt vinkelrett på' disse og to ytterligere sider som praktisk talt danner en vinkel på 45° med den tredje side og hvor det på to av sidene er anordnet en inngangs- resp. utgangsomformer. Slike anordninger anvendes f.eks. for forsinkelse av videosignaler, hvilket er nodvendig i forskjellige fargefjernsynssystemer. Ultralyd-svingningene underkastes gjentatte refleksjoner på prismets sideflater slik at et prisme med forholdsvis små dimensjoner kan gi en tilstrekke-lig forsinkelsestid. De vanlige forsinkelsesanordninger har den ulempe at det må stilles meget store krav til nøyaktigheten av prismets ut-fbrelse for å sikre pålitelig drift. The invention relates to an ultrasonic delay device with a prism-shaped medium with a substantially pentagonal base surface and which is formed by two practically parallel sides, a third side which is practically perpendicular to these and two further sides which practically form an angle of 45° with the third side and where there is an entrance or output converter. Such devices are used e.g. for delaying video signals, which is necessary in various color television systems. The ultrasound oscillations are subjected to repeated reflections on the prism's side surfaces so that a prism with relatively small dimensions can provide a sufficient delay time. The usual delay devices have the disadvantage that very high demands must be made on the accuracy of the prism's production in order to ensure reliable operation.
Hensikten med oppfinnelsen er å tilveiebringe en anordning hvor forsinkelsesmediet kan ha betydelige formtoleranser. The purpose of the invention is to provide a device where the delay medium can have significant shape tolerances.
På den måte kan det fremstilles forholdsvis billig,f.eks. av pressglass med liten eller sågar uten noen som helst etterbehandling. In that way, it can be produced relatively cheaply, e.g. of pressed glass with little or even no finishing.
Dette oppnås ifolge oppfinnelsen ved at inngangs- According to the invention, this is achieved by input
og utgangsomformeren er anordnet på hver sin side av de to -ytterligere sider, og at lengden av de to parallelle sider er valgt slik at fra and the output converter is arranged on each side of the two -further sides, and that the length of the two parallel sides is chosen so that from
ii^i^tn^g^nip rine ren utstrålte ultralydbolger som treffer de parallelle .si(f&»>*eFlékterés" to ganger fra hver av'disse sider for- de treffer^tJgMigsomforme-ren. ' : . f ..Et utforelseseksempel pa oppfinnelsen skal forklares nærmere undei> henvisning til tegningen som viser et grunnriss av en anordning ifolge oppfinnelsen." , . Ultralydforsinkelseslegemet L består av et egnet medium, f.eks. glass, særlig pressglass, og har form av et prisme med ^emk&ntet grunnflate.. Prismet har to -parallelle sider 1 og 2, en tredje eide 3 som står tilnærmet vinkelrett på sidene 1. og 2 og en fjerde og femte side 4 resp. 5 som danner en vinkel på praktisk talt 45° med den tredje side 3* I tilfélie mediet er pressglass er hjornene i femkanten noe avrundet. Sidér.ne^°65 baerér. en .Inngangs- resp. en utgangsomformer resp, T^.av et "eller annet piezo-elektrisk materiale, f.eks. polarisert bariunjtitanat. Xerigden ay. sidene 1 og 2 er valgt slik at mekaniske fra omformere^.T-^u,.ts.trålte ultralydsvingninger (særlig svingninger.hvis-^Yih^ningsretning ikke bare står vinkelrett på utbre-delsesrétningen,'men også-Vinkelrett på femkantens plan) etter hver-andre reflekteres på siden 2 og siden 1 og siden 3°6igjen-siden 2 og siden 1 for den treffer utgangsomforméren Tg i samme fase«.Lengden av sidene 1 og 2-er fortrinnsvis :to ganger stbrre enn lengden.av siden 3.».På - hver^ "av-'Sidene* ;l' bg 2 opptrer derfor to ganger refleksjon. _t'<*->■ • Ved. en slik «oppbygning er små avvikelser i hjornene me ULorn sidene 1 og- 2 og de øvrige sider tillatt uten at anordningen -blir ubrukelig av tien grunn'.' Dette kan forklares" på fblgende måte: u - Hvis d«t. antas at sideflaten 1 ikke er slik s,om vist "på tegningen fted op^tfrujche linjer, men derimot som antydet med den stfékede linje l1 , vil "'tilt ra lyd svingningene Ikke reflekteres slik som vist med opptrukken linje o, <ne<*>n slik .som vist. med streket linje b'. Avvikélaen mellom sidene,, 1 ojg i' er béregnet med ( f ag avvikelsen mellom linjen 6' og 6 er.da 2 y . Det samme gjelder foT den reflekterte bblge på platen 3 som ikke lenger folger den opptrukne linje 7» men linjen 7' som også avviker fra en vinkel 2^fra linjen 7. Dette gjelder også for de bvrige refleksjonslinjer 8 resp. 8' og 9 resp. 9'°6man ser at i begge tilfeller vil den reflekterte bblge 9 resp. 9' treffe omformeren T^på den femte side 5-Herav fremgår at en vinkelavvkkelse av siden 1' har tilfblge" at den utstrålte ultralydbblge forskyves noe uten at dette gjor seg gjeldende på driftsresultatet. Så lenge•vinkeltoleransen for ii^i^tn^g^nip rine purely radiated ultrasound waves that hit the parallel .si(f&»>*eFlékterés" twice from each of these sides before they hit the tJgMigsomformer-ren. ' : . f ..An embodiment of the invention shall be explained in more detail with reference to the drawing which shows a plan view of a device according to the invention." prism with a defined base. The prism has two -parallel sides 1 and 2, a third side 3 which is approximately perpendicular to sides 1 and 2 and a fourth and fifth side 4 and 5 respectively which form an angle of practically 45° with the third side 3* If the medium is pressed glass, the corners of the pentagon are somewhat rounded. The 65° sides bear an input or an output converter or T of a "or other piezoelectric material, f .ex. polarized barium titanate. Xerigden ay. sides 1 and 2 are chosen so that mechanical ultrasonic oscillations transmitted from transducers (especially oscillations whose direction of propagation is not only perpendicular to the direction of propagation, but also perpendicular to the plane of the pentagon ) after each other is reflected on side 2 and side 1 and side 3°6again-side 2 and side 1 because it hits the output transformer Tg in the same phase". The length of sides 1 and 2 is preferably :twice as long as the length of side 3.». On - each^ "of-'The sides* ;l' bg 2 therefore occurs twice reflection. _t'<*->■ • With. such a "structure there are small deviations in the corners with ULorn sides 1 and - 2 and the other pages allowed without the device -becoming unusable for ten reasons'.' This can be explained" in the following way: u - If d«t. it is assumed that the side surface 1 is not as shown "on the drawing with vertical lines, but on the other hand, as indicated by the broken line l1, the sound vibrations will not be reflected as shown by the solid line o, <ne< *>n such .as shown. with dashed line b'. The deviation between the sides ,, 1 and i' is calculated with ( f ag the deviation between the line 6' and 6 is then 2 y . The same applies to the reflected bblge on the plate 3 which no longer follows the drawn line 7" but the line 7 ' which also deviates from an angle 2^ from the line 7. This also applies to the other reflection lines 8 and 8' and 9 and 9'°6 it can be seen that in both cases the reflected beam 9 and 9' will hit the converter T ^on the fifth side 5-From this it appears that an angular deviation of the side 1' has caused" that the radiated ultrasound beam is displaced somewhat without this affecting the operating result. As long as the angular tolerance for
siden 1 er "liten og eventuelt også for siden 2, skjer korreksjon altså ' automatisk^ hvis antallet ref lekajaner.,,bibeholdes. side 1 is "small and possibly also for side 2, correction therefore takes place 'automatically' if the number of reference boxes is maintained.
Ved et utforelseeeksempel med et legeme L av pressglass med en utbredelseshast^ighét på 2500 m/sek, hadde sidene 1 og 2 en lengde på ca. 50 mm ,,og siden 3 en lengde på ca. 25 mm. For-sinkelsestiden var 64 yusek som er bnskelig for fargefjernsynssystemer. In an exemplary embodiment with a body L of pressed glass with a propagation speed of 2500 m/sec, sides 1 and 2 had a length of approx. 50 mm, and side 3 a length of approx. 25 mm. The delay time was 64 yusec which is desirable for color television systems.
Claims (1)
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NL656504937A NL143392B (en) | 1965-04-17 | 1965-04-17 | ULTRASONIC DELAYER. |
Publications (1)
Publication Number | Publication Date |
---|---|
NO116769B true NO116769B (en) | 1969-05-19 |
Family
ID=19792967
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
NO162581A NO116769B (en) | 1965-04-17 | 1966-04-14 |
Country Status (12)
Country | Link |
---|---|
US (1) | US3475704A (en) |
AT (1) | AT261000B (en) |
BE (1) | BE679636A (en) |
CH (1) | CH435828A (en) |
DE (1) | DE1616677B1 (en) |
DK (1) | DK119835B (en) |
ES (1) | ES128244Y (en) |
FI (1) | FI44172B (en) |
GB (1) | GB1083531A (en) |
NL (1) | NL143392B (en) |
NO (1) | NO116769B (en) |
SE (1) | SE317708B (en) |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE1596845B1 (en) * | 1966-12-07 | 1970-10-22 | Jenaer Glaswerk Schott & Gen | Glass with a small temperature coefficient of travel time for ultrasonic waves |
DE1696064A1 (en) * | 1968-03-08 | 1972-03-09 | Jenaer Glaswerk Schott & Gen | GLASSES FOR ULTRASONIC DELAY CABLES WITH LOWER INTERNAL DAMPING AND TRANSFORMATION TEMPERATURES BETWEEN 550 AND 620 DEGREES C. |
NL6817492A (en) * | 1968-12-06 | 1969-02-25 | ||
DE3206452A1 (en) * | 1982-02-23 | 1983-09-01 | Siemens AG, 1000 Berlin und 8000 München | ULTRASONIC DELAY LINE AND METHOD FOR THE PRODUCTION THEREOF |
DE3206401A1 (en) * | 1982-02-23 | 1983-09-01 | Siemens AG, 1000 Berlin und 8000 München | "ULTRASONIC DELAY LINE" |
US4488128A (en) * | 1983-04-22 | 1984-12-11 | Gte Products Corporation | Bifurcated electroacoustic delay line with diagonal coupling |
US4525692A (en) * | 1983-04-22 | 1985-06-25 | Gte Products Corporation | Electroacoustic delay lines |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2839731A (en) * | 1953-01-14 | 1958-06-17 | Bell Telephone Labor Inc | Multi-facet ultrasonic delay line |
NL297704A (en) * | 1962-09-26 |
-
1965
- 1965-04-17 NL NL656504937A patent/NL143392B/en unknown
-
1966
- 1966-03-31 US US539191A patent/US3475704A/en not_active Expired - Lifetime
- 1966-04-13 DE DE1966N0028377 patent/DE1616677B1/en not_active Withdrawn
- 1966-04-14 FI FI0966/66A patent/FI44172B/fi active
- 1966-04-14 CH CH538766A patent/CH435828A/en unknown
- 1966-04-14 NO NO162581A patent/NO116769B/no unknown
- 1966-04-14 GB GB16419/66A patent/GB1083531A/en not_active Expired
- 1966-04-14 DK DK193166AA patent/DK119835B/en unknown
- 1966-04-14 AT AT352266A patent/AT261000B/en active
- 1966-04-14 SE SE5111/66A patent/SE317708B/xx unknown
- 1966-04-15 BE BE679636D patent/BE679636A/xx unknown
- 1966-04-15 ES ES128244U patent/ES128244Y/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
BE679636A (en) | 1966-10-17 |
NL6504937A (en) | 1966-10-18 |
FI44172B (en) | 1971-06-01 |
DK119835B (en) | 1971-03-01 |
AT261000B (en) | 1968-04-10 |
GB1083531A (en) | 1967-09-13 |
US3475704A (en) | 1969-10-28 |
DE1616677B1 (en) | 1970-10-22 |
ES128244Y (en) | 1967-12-16 |
SE317708B (en) | 1969-11-24 |
ES128244U (en) | 1967-07-01 |
NL143392B (en) | 1974-09-16 |
CH435828A (en) | 1967-05-15 |
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