US3651431A - Zero temperature coefficient ultrasonic transmission medium having temporal stability - Google Patents

Zero temperature coefficient ultrasonic transmission medium having temporal stability Download PDF

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US3651431A
US3651431A US821693A US3651431DA US3651431A US 3651431 A US3651431 A US 3651431A US 821693 A US821693 A US 821693A US 3651431D A US3651431D A US 3651431DA US 3651431 A US3651431 A US 3651431A
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John T Krause
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    • C—CHEMISTRY; METALLURGY
    • C03—GLASS; MINERAL OR SLAG WOOL
    • C03C—CHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C3/00—Glass compositions
    • C03C3/04—Glass compositions containing silica
    • C03C3/076—Glass compositions containing silica with 40% to 90% silica, by weight
    • C03C3/102—Glass compositions containing silica with 40% to 90% silica, by weight containing lead
    • C—CHEMISTRY; METALLURGY
    • C03—GLASS; MINERAL OR SLAG WOOL
    • C03C—CHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C4/00—Compositions for glass with special properties
    • C03C4/0057—Compositions for glass with special properties for ultrasonic delay lines glass
    • H—ELECTRICITY
    • H03—ELECTRONIC CIRCUITRY
    • H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/30—Time-delay networks
    • H03H9/36—Time-delay networks with non-adjustable delay time

Definitions

  • An ultrasonic delay line having as the delay medium a glass of the nominal composition in mole per cent 17 per cent lead oxide, 95 per cent barium oxide and 73.5 per cent silicon dioxide, exhibits an average temperature coefiicient of delay time 1 of not more than about :5 parts per million per degrees centigrade over the range 0 to 100 C., a thermal after-efi'ect of not more than about 10 p.p.m., and an aging of delay time of not more than -10 parts per million per decade (decade is an order of magnitude of time in days).
  • T.C. temperature coefficient
  • a new glass ultrasonic transmission medium has been discovered, which has the nominal composition in mole per cent 17 per cent lead oxide, 9.5 per cent barium oxide and 73.5 per cent silicon dioxide.
  • This glass not only exhibits near zero temperature coefficient of delay time over the normally encountered temperature range of 0 to 100 C., but also exhibits substantial independence of thermal after-effects and of aging of delay time with the thermal history. That is, the thermal after-effect is not greater than p.p.m. and the aging of delay time is less than l0 parts per million per decade of time, regardless of prior thermal treatment, thus making the glass suitable for critical ultrasonic applications, such as the delay medium in ultrasonic delay lines, without the need for a final thermal treatment of the glass.
  • FIG. 1 is a graph depicting BaO-PbO-SiO, glass compositions which are useful as ultrasonic transmission media according to the invention
  • FIG. 2 is a schematic illustration of a delay line assembly incorporating the inventive material as a delay medium.
  • FIG. 1 graphically illustrates the family of BaO-PbO-SiO, glasses which exhibit an average temperature coefficient of delay time of a maximum of :5 parts per million per degrees centigrade over the range 0 to 100 C. It has been determined that this family of glasses exhibit thermal after-effects not greater than 10 ppm. and an aging of delay time (temporal instability) of not more than l0 parts per million per decade.
  • the average temperature coefficient of delay time from 0 to 100 C. is plotted along the vertical axis and the mole ratio of PhD to [PhD Si0,] is plotted along the horizontal axis for three different series of compositions, each having a different 2. 11.0 mole percent BaO, 0.189 mole ratio PbO/[Pb0+ SiO,] and 8.0 mole percent BaO, 0.221 mole ratio PbO/[ 2];
  • compositions fall within a much broader glass-forming region of the ternary diagram roughly defined by the ranges in mole per cent 0 to 40 BaO, 0m 60 PbO and 40 to SiO, Within this parallelogram, the thermal after-effect and the aging of delay time is substantially independent of the glasses thermal histories and does not exceed 10 p.p.m. and -l0 parts per million per decade respectively. Varying the BaO content so as to result in compositions outside the parallelogram adjacent to lines B or C may result in devitrification of the melt. Increasing the PbO content at the expense of S10, increases the temperature coefficient of delay time linearly, as may be seen from FIG. 1.
  • compositions within the parallelogram defined by lines B, C, F and G are preferred for their average temperature coefficients of delay time of not more than :2 parts per million per degrees centigrade. These compositions fall within an area of the ternary diagram formed by connecting with straight lines the following point pairs:
  • minor amounts of additives or impurities, exclusive of the Group I alkali metals Li, Na, K, Rb, Cs, typically up to about 1 mole per cent total, may be present in the glass compositions without adversely affecting the acoustic properties.
  • fining agents such as Asp, or Sb,0 typically up to 1 mole per cent may be present.
  • the alkali metals should not be present in amounts greater than about 0.1 cation per cent, in order to avoid adverse thermal after-effects or aging.
  • the described glasses may be produced in any suitable manner known to the glass-making art, although some advantage may be gained by following the known methods of producing optical quality glass. Also a fine anneal may be desirable in reducing the level of acoustic loss. Although not a necessary part of this description, a fine anneal is described in US. Pat. No. 3,173,780, issued to H. C. Hoover on Mar. 16, 1965.
  • the molten glass may be shaped into blanks having roughly the desired form and subsequently finished by the usual cutting, grinding and polishing steps.
  • the blanks may be annealed according to steps known in the glass-making art.
  • thermal after-effects and temporal instabilities are minimal and are substantially unaffected by the character of the anneal or other prior or post-thermal treatment.
  • Samples suitable for the obtaining of acoustic properties were prepared by optically polishing flat and parallel the opposite ends of %-inch diameter right cylinders 1 inch in length. These were processed into one-ended delay lines and measured for the appropriate acoustic properties using pulse-echo techniques. The thermal aftereffect was determined by measuring the unit delay time at 25 C. before and after an 18- hour soak at 125 C. Temporal instability was then measured at 25 C. as a function of time over a several-hundred-day period.
  • Shear Delay Time Temporal instability Thermal After-effect Temperature Coeflicient of Delay Time (from C. to 100 C.) Shear Attenuation (at 50 MHz) 2.5 decibels/centimeter Frequency Dependency of ,1.3
  • a solid ultrasonic delay line comprising a solid ultrasonic transmission medium, means for converting electrical signals to acoustic pulses comprising two piezoelectric transducers affixed to opposite faces of said medium, and electrical input and output means attached to said transducers, characterized in that said transmission medium is a bariumlead-silicate glass having an average temperature coefficient of delay time of up to 5 parts per million per degrees centigrade, a thermal after-effect of less than 10 parts per million per decade and consisting essentially of a composition within an area of the .ternary diagram for barium oxide, lead oxide and silicon dioxide formed by connecting with straight lines the following point pairs:
  • said transmission medium additionally containing up to one percent of one or more fining agents selected from the group consisting of AS203 and Sb O and not more than one-tenth cation percent of the Group I alkali metals.

Abstract

An ultrasonic delay line, having as the delay medium a glass of the nominal composition in mole per cent 17 per cent lead oxide, 95 per cent barium oxide and 73.5 per cent silicon dioxide, exhibits an average temperature coefficient of delay time of not more than about + OR - 5 parts per million per degrees centigrade over the range 0* to 100* C., a thermal after-effect of not more than about 10 p.p.m., and an aging of delay time of not more than -10 parts per million per decade (decade is an order of magnitude of time in days).

Description

United States Patent Krause 1451 Mar. 21, 1972 [73] Assignee: Bell Telephone Laboratories, Incorporated, Murray Hill, Berkeley Heights, NJ.
22 Filed: May 5,1969
21 Appl.No.: 821,693
[52] U.S. Cl. ..333/30 R, 106/53 [51] Int. Cl "1103f 3/68, C036 3/04, CO3c 3/10 [58] Field of Search 106/53; 333/30 [56] References Cited- UNlTED STATES PATENTS 3,154,425 10/1964 Hoover et a1. 106/53 FOREIGN PATENTS OR APPLICATIONS 1,118,422 6/1968 GreatBritain....,... .106/53 1,383,962 11/1963 France ..l06/53 OTHER PUBLICATIONS Argyle, J. F. and Hummel, F. A., The. System PhD- 8110- MgO-Si0 1, Phase Studies in Subsidiary Ternary Systems.
Glasslndustry 46(10) pp. 583- 587 and 62 7,1965 October.
Primary Examiner-Tobias E. Levow Assistant Examiner-M. Bell Attorney-R. J. Guenther and Edwin B. Cave [5 7] ABSTRACT An ultrasonic delay line, having as the delay medium a glass of the nominal composition in mole per cent 17 per cent lead oxide, 95 per cent barium oxide and 73.5 per cent silicon dioxide, exhibits an average temperature coefiicient of delay time 1 of not more than about :5 parts per million per degrees centigrade over the range 0 to 100 C., a thermal after-efi'ect of not more than about 10 p.p.m., and an aging of delay time of not more than -10 parts per million per decade (decade is an order of magnitude of time in days).
3 Claims, 2 Drawing Figures PATENTEDMARZI 1922 AVERAGE T.C. DELAY TIME (o-|ooc) IN PPm/c I l l I L l P.b0 X MOLE RATIO PbOJrSiOZ I00 INVENTOR J. 7. KRAUSE NEY ZERO TEMPERATURE COEFFICIENT ULTRASONIC TRANSMISSION MEDIUM HAVING TEMPORAL STABILITY FIELD OF THE INVENTION This invention relates to a glass ultrasonic transmission medium having both high temporal stability and temperature stability of delay time, and to ultrasonic devices utilizing same.
PRIOR ART Many applications being considered for ultrasonic delay lines require a unit delay time which is stable with time over the nonnally encountered temperature range. Various glass delay media are known which have near zero temperature coefficients of delay time falling within the temperature range of normal use to 100 C. Among these are the alkali-leadsilicate glasses described in U.S. Pat. No. 3,154,425 issued to H. L. Hoover and M. E. Nordberg on Oct. 27, 1964, and having average temperature coefficients of delay time of up to 8 parts per million per degrees centigrade.
However, when changes in delay time from all sources are considered, a temperature coefficient (T.C.) of as little as :8 parts per million per degrees centigrade over the range of 0 to 100 C. may be too high for the most critical applications. Moreover, these near zero T.C. glasses have been found to exhibit changes in unit delay time resulting from thermal aftereffects of up to several hundred parts per million and from temporal instability effects (aging) of up to 40 parts per million per decade. (This latter number has been arrived at by plotting change in delay time in parts per million versus days on a log scale. For convenience, the term decade as used herein is intended to refer to the number of days along this log scale.) This amount of variation in delay time is a considerable contribution to the overall change in unit delay time tolerable, and thus too high for some critical applications. In the case of the alkali-lead-silicate glasses mentioned, it has been found that these instability characteristics are related to the glasses thermal histories. This problem is treated in U. S. Pat. No. 3,173,780 issued to H. L. Hoover on Mar. 16, 1965, which describes a thermal treatment to reduce the propensity of the glass toward temporal changes or aging of delay time. As an additional step this thermal treatment to reduce aging is, of course, undesirable, since it increases the cost of producing the delay medium. Furthermore, it has been found that a moderately fine anneal results in less aging than a coarse anneal. The additional control required to achieve the fine anneal further increases the cost of producing the glass delay medium.
SUMMARY OF THE INVENTION A new glass ultrasonic transmission medium has been discovered, which has the nominal composition in mole per cent 17 per cent lead oxide, 9.5 per cent barium oxide and 73.5 per cent silicon dioxide. This glass not only exhibits near zero temperature coefficient of delay time over the normally encountered temperature range of 0 to 100 C., but also exhibits substantial independence of thermal after-effects and of aging of delay time with the thermal history. That is, the thermal after-effect is not greater than p.p.m. and the aging of delay time is less than l0 parts per million per decade of time, regardless of prior thermal treatment, thus making the glass suitable for critical ultrasonic applications, such as the delay medium in ultrasonic delay lines, without the need for a final thermal treatment of the glass.
BRIEF DESCRIPTION OF THE DRAWING FIG. 1 is a graph depicting BaO-PbO-SiO, glass compositions which are useful as ultrasonic transmission media according to the invention;
FIG. 2 is a schematic illustration of a delay line assembly incorporating the inventive material as a delay medium.
DETAILED DESCRIPTION OF THE INVENTION FIG. 1 graphically illustrates the family of BaO-PbO-SiO, glasses which exhibit an average temperature coefficient of delay time of a maximum of :5 parts per million per degrees centigrade over the range 0 to 100 C. It has been determined that this family of glasses exhibit thermal after-effects not greater than 10 ppm. and an aging of delay time (temporal instability) of not more than l0 parts per million per decade. The average temperature coefficient of delay time from 0 to 100 C. is plotted along the vertical axis and the mole ratio of PhD to [PhD Si0,] is plotted along the horizontal axis for three different series of compositions, each having a different 2. 11.0 mole percent BaO, 0.189 mole ratio PbO/[Pb0+ SiO,] and 8.0 mole percent BaO, 0.221 mole ratio PbO/[ 2];
3. 8.0 mole percent BaO, 0.221 mole ratio PbO/[PbO+SiO and 8.0 mole percent BaO, 0.187 mole ratio PbO/[P- bO+SiO,];
4. 8.0 mole percent BaO, 0.187 mole ratio PbO/[PbO+SiO and 11.0 mole percent BaO, 0.155 mole ratio PbO/[P- bO+SiO,].
These compositions fall within a much broader glass-forming region of the ternary diagram roughly defined by the ranges in mole per cent 0 to 40 BaO, 0m 60 PbO and 40 to SiO, Within this parallelogram, the thermal after-effect and the aging of delay time is substantially independent of the glasses thermal histories and does not exceed 10 p.p.m. and -l0 parts per million per decade respectively. Varying the BaO content so as to result in compositions outside the parallelogram adjacent to lines B or C may result in devitrification of the melt. Increasing the PbO content at the expense of S10, increases the temperature coefficient of delay time linearly, as may be seen from FIG. 1. Varying the PbO/[PbO $10,] content so as to result in compositions outside the parallelogram adjacent lines D or E of course results in average temperature coefficients of delay time in excess of 2-5 parts per million per degrees centigrade, which is too high for many ultrasonic applications. For the most critical applications, compositions within the parallelogram defined by lines B, C, F and G are preferred for their average temperature coefficients of delay time of not more than :2 parts per million per degrees centigrade. These compositions fall within an area of the ternary diagram formed by connecting with straight lines the following point pairs:
1. 11.0 mole percent BaO, 0.166 mole ratio PbO/[Pb0+ SiO and 11.0 mole percent BaO, 0.177 mole ratio P zl;
2. 11.0 mole percent BaO,-0.177 mole ratio PbO/[Pb0+ SiO and 8.0 mole percent BaO, 0.209 mole ratio ll zl;
3. 8.0 mole percent BaO, 0.209 mole ratio PbO/[PbO-i-SiO, and 8.0 mole percent BaO, 0.199 mole ratio PbO/[l bO+SiO 4. 8.0 mole percent BaO, 0.199 mole ratio PbO/[PbO+SiO,
] and 11.0 mole percent BaO, 0.166 mole ratio PbO/[P- b0+SiO,].
In general, minor amounts of additives or impurities, exclusive of the Group I alkali metals Li, Na, K, Rb, Cs, typically up to about 1 mole per cent total, may be present in the glass compositions without adversely affecting the acoustic properties. For example, fining agents such as Asp, or Sb,0 typically up to 1 mole per cent may be present. The alkali metals should not be present in amounts greater than about 0.1 cation per cent, in order to avoid adverse thermal after-effects or aging.
The described glasses may be produced in any suitable manner known to the glass-making art, although some advantage may be gained by following the known methods of producing optical quality glass. Also a fine anneal may be desirable in reducing the level of acoustic loss. Although not a necessary part of this description, a fine anneal is described in US. Pat. No. 3,173,780, issued to H. C. Hoover on Mar. 16, 1965.
The molten glass may be shaped into blanks having roughly the desired form and subsequently finished by the usual cutting, grinding and polishing steps. The blanks may be annealed according to steps known in the glass-making art. However, as already noted, thermal after-effects and temporal instabilities are minimal and are substantially unaffected by the character of the anneal or other prior or post-thermal treatment.
EXAMPLE:
A glass having the final composition in mole per cent of 73.45 SiO,, 17.05 PbO, 9.50 BaO, was melted in a 34-inch clay pot, into which 1 mole per cent As O was added as a fining agent. Additional fining and oxidizing action was obtained by adding 4 weight per cent of the BaO in the form of Ba(NO The remainder of BaO was added as BaCO Samples suitable for the obtaining of acoustic properties were prepared by optically polishing flat and parallel the opposite ends of %-inch diameter right cylinders 1 inch in length. These were processed into one-ended delay lines and measured for the appropriate acoustic properties using pulse-echo techniques. The thermal aftereffect was determined by measuring the unit delay time at 25 C. before and after an 18- hour soak at 125 C. Temporal instability was then measured at 25 C. as a function of time over a several-hundred-day period.
The following table sets forth the thermal after-effect and temporal instability of delay time as determined by the above procedure, together with some other significant acoustic properties obtained for these samples.
9.67 microseconds/inch less than 5 p.p.m./decade less than 10 p.p.m.
less than one part per million per C.
Shear Delay Time Temporal instability Thermal After-effect Temperature Coeflicient of Delay Time (from C. to 100 C.) Shear Attenuation (at 50 MHz) 2.5 decibels/centimeter Frequency Dependency of ,1.3
Shear Loss Mechanical impedance 9.7 X 10 g.lcm.sec. Density 3.7 g.lcc.
gular, polygonal or other delay medium shape, known or unknown.
What is claimed is: l. A solid ultrasonic delay line comprising a solid ultrasonic transmission medium, means for converting electrical signals to acoustic pulses comprising two piezoelectric transducers affixed to opposite faces of said medium, and electrical input and output means attached to said transducers, characterized in that said transmission medium is a bariumlead-silicate glass having an average temperature coefficient of delay time of up to 5 parts per million per degrees centigrade, a thermal after-effect of less than 10 parts per million per decade and consisting essentially of a composition within an area of the .ternary diagram for barium oxide, lead oxide and silicon dioxide formed by connecting with straight lines the following point pairs:
1. 11.0 mole percent BaO, 0.155 mole ratio PbO/[PbO'i- SiO,] and 11.0 mole percent BaO, 0.189 mole ratio PbO/[PbO+ 2. 11.0 mole percent BaO, 0.189 mole ratio PbO/[Pb0+ SiO,] and 8.0 mole percent- BaO, 0.221 mole ratio PbO/[PbO-i- 3. 8.0 mole percent BaO, 0.221 mole ratio PbO/[PbO+SiO,
] and 8.0 mole percent BaO, 0.187 mole ratio PbO/[P- bO+SiO 4. 8.0 mole percent BaO, 0.187 mole ratio PbO/[PbO-i-SiO and 11.0 mole percent BaO, 0.155 mole ratio PbO/[P- bO+SiO- t];
said transmission medium additionally containing up to one percent of one or more fining agents selected from the group consisting of AS203 and Sb O and not more than one-tenth cation percent of the Group I alkali metals.
2. The solid ultrasonic delay line of claim 1 in which the transmission medium is a glass consisting essentially of a composition within an area of the ternary diagram for barium oxide, lead oxide, and silicon dioxide, formed by connecting with straight lines the following point pairs:
1. 11.0 mole percent BaO, 0.166 mole ratio PbO/[Pb0+ SiO and 11.0 mole percent BaO, 0.177 mole ratio ll zl;
2. 11.0 mole percent BaO, 0.177 mole ratio PbO/[Pb0+ SiO,] and 8.0 mole percent BaO, 0.209 mole ratio PbOll zi;
3. 8.0 mole percent BaO, 0.209 mole ratio PbO/[PbO+SiO 1 and 8.0 mole percent BaO, 0.199 mole ratio PbO/[P- bO+SiO 4. 8.0 mole percent BaO, 0.199 mole ratio PbO/[PbO+SiO and 11.0 molepercent BaO, 0.166 mole ratio PbO/[P- bO-l-SiO said transmission medium additionally containing up to one percent-of one or more fining agents selected from the group consisting of Asp. and Sb O and not more than one-tenth cation percent of the Group 1 alkali metals.
3. The solid ultrasonic delay line of claim 1 in which the transmission medium is a glass consisting essentially of a composition in mole percent of 73.45 percent SiO 17.05 percent PbO, 9.50 percent BaO.

Claims (8)

  1. 2. The solid ultrasonic delay line of claim 1 in which the transmission medium is a glass consisting essentially of a composition within an area of the ternary diagram for barium oxide, lead oxide, and silicon dioxide, formed by connecting with straight lines the following point pairs:
  2. 2. 11.0 mole percent BaO, 0.177 mole ratio PbO/(PbO+SiO2) and 8.0 mole percent BaO, 0.209 mole ratio PbO/(PbO+SiO2);
  3. 2. 11.0 mole percent BaO, 0.189 mole ratio PbO/(PbO+SiO2) and 8.0 mole percent BaO, 0.221 mole ratio PbO/(PbO+SiO2);
  4. 3. 8.0 mole percent BaO, 0.221 mole ratio PbO/(PbO+SiO2) and 8.0 mole percent BaO, 0.187 mole ratio PbO/(PbO+SiO2);
  5. 3. The solid ultrasonic delay line of claim 1 in which the transmission medium is a glass consisting essentially of a composition in mole percent of 73.45 percent SiO2, 17.05 percent PbO, 9.50 percent BaO.
  6. 3. 8.0 mole percent BaO, 0.209 mole ratio PbO/(PbO+SiO2) and 8.0 mole percent BaO, 0.199 mole Ratio PbO/(PbO+SiO2);
  7. 4. 8.0 mole percent BaO, 0.199 mole ratio PbO/(PbO+SiO2) and 11.0 mole percent BaO, 0.166 mole ratio PbO/(PbO+SiO2); said transmission medium additionally containing up to one percent of one or more fining agents selected from the group consisting of As2O3 and Sb2O3, and not more than one-tenth cation percent of the Group I alkali metals.
  8. 4. 8.0 mole percent BaO, 0.187 mole ratio PbO/(PbO+SiO2) and 11.0 mole percent BaO, 0.155 mole ratio PbO/(PbO+SiO2); said transmission medium additionally containing up to one percent of one or more fining agents selected from the group consisting of As2O3 and Sb2O3, and not more than one-tenth cation percent of the Group I alkali metals.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3783416A (en) * 1969-12-22 1974-01-01 Owens Illinois Inc Solid ultrasonic delay lines and glass compositions therefor

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5341526U (en) * 1976-09-14 1978-04-10

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3154425A (en) * 1961-06-19 1964-10-27 Corning Glass Works Temperature stable ultrasonic delay lines
FR1383962A (en) * 1962-11-30 1965-01-04 Western Electric Co Ultrasonic delay line
GB1118422A (en) * 1965-04-15 1968-07-03 Philips Electronic Associated Improvements relating to acoustic delay lines

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3154425A (en) * 1961-06-19 1964-10-27 Corning Glass Works Temperature stable ultrasonic delay lines
FR1383962A (en) * 1962-11-30 1965-01-04 Western Electric Co Ultrasonic delay line
GB1118422A (en) * 1965-04-15 1968-07-03 Philips Electronic Associated Improvements relating to acoustic delay lines

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
Argyle, J. F. and Hummel, F. A., The System PbO BaO MgO SiO 2 I, Phase Studies in Subsidiary Ternary Systems, Glass Industry 46(10) pp. 583 587 and 627, 1965 October. *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3783416A (en) * 1969-12-22 1974-01-01 Owens Illinois Inc Solid ultrasonic delay lines and glass compositions therefor

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DE2022046B2 (en) 1971-10-21
NL7006344A (en) 1970-11-09
FR2047280A5 (en) 1971-03-12

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