US1996359A - Photographic recording of acoustic or the like oscillations - Google Patents
Photographic recording of acoustic or the like oscillations Download PDFInfo
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- US1996359A US1996359A US370107A US37010729A US1996359A US 1996359 A US1996359 A US 1996359A US 370107 A US370107 A US 370107A US 37010729 A US37010729 A US 37010729A US 1996359 A US1996359 A US 1996359A
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- oscillations
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- light
- acoustic
- frequency
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
Definitions
- Fig. 5 illustrates the methOd-,accordingto the presentinventionin 'which the two oscillations of Figs. 1 and ⁇ 2 arev added together. It will be no- UNITED STAT ENT 'O FICE
- the present invention relates, to the production ,of a light beam having an intensity which varies in accordance with acoustic OI' the like oscillations; more particularly for the photographic 'Where high frequency.
- electrical oscillation modulated With acoustic currents are used to light a discharge tube the total light emitted by the tube, varies in accordance with the modulation, Since modulation of high frequency oscillations consists in varying, the amplitude of these oscillations in accordance with the acoustic currents.
- a' glow discharge tube is employed andto the electrodes thereof are applied two sets of electrical oscillations, one set of oscillations being of substantially constant amplitude and frequency and the other set of oscillations corresponding to the oscillations in accordance with which the light intensity is to be varied.
- the light emitted tained its constant amplitude but that, in effect, the center line OX in Fig. 1 has in Fig. 5 been deformed into 'the shape of the low frequency curve in Fig. 2.
- the light emitted by one electrode is a function of the shaded area above the line OX while that emitted by the other electrode is a function" of ⁇ the shaded area below the line OX.
- the intensity of the light emitted by the former electrode is indicated'by the plain dotted curve trode is .indicated by thechain dotted curve b.
- the total light emittedby the lamp is the sum of 'these twodotted curves and is represented by though the intensity of the light emitted by each ofthe electrodes -separately 'varies inaccordance with the low frequency oscillation in Fig; 2, that the tube, taken separately, is varied in accordan emitted' by the lamp as awhole is of much smaller with the oscillations to be recorded.
- Figs. 1-6 are diagrams illustrating the method of the present invention in contrast With the known method using modulated high. frequency oscillations, and 4 Fig. 'lis a Circuit' dia the invention. y i
- a suitable Circuit A for. carrying; the present, inventioninto effect is shown -in v Fig 7.
- High frequency oscillations are ed into the primary winding of thetransformer .d and the low frequency oscillations are fed intothe- 'primary winding ⁇ of :the transformer e.
- a condenser f serves to prevent lowfrequency oscillations from circulating in' the Circuit tothe left of the glow disch'arge 'tube g while a high frequency choke coil h prevents high frequency oscillations from circulating in the Circuit to the right of the discharge tube g.
- the oscillations of constant frequency and amplitude have, preferably, a frequency above audibility but they may have an audible frequency to which the appara'tus is not sensitive.
- an optical slit is used for recording oscillations, it can be shown that when the ripple wave'length of the oscillations (that is to say' gram 'in accordance with age of the other electrode is plotted as ordinate, the line .OX representing Zero voltage and positive voltages being plotted in an upward direction.
- light intensity is plotted as ordinate, the axis OXrepreSenting Zero intensity.
- time is plotted as abscissa, the Scale being uniform in all the figures.
- the high frequency ripple is disregarded in Figs. 4 and 6.
- Fig. 1 shows a high frequency oscillation of constant amplitude and Fig. 2 shows one complete period of a low frequency oscillation with which it is desired to modulate the intensity of the light emitted by the glow discharge tube.
- Fig. 3 illustrates the effect of modulating the oscillation of Fig. 1 by that of Fig. 2, the amplitude of the high frequency oscillation being varied in accordance with the low frequency oscillation.
- the total light emitted by the tube is a function of the total shaded area irrespective of which or shade upon the record) is equal to the'slit Width, no Variation in the light transmitted by the slit takes place.
- the apparatus therefore, shows no response and is insensitive to the frequency corresponding to this wave length.
- oscillations of this frequency can be used in combination With the oscillations to be recorded as above described.
- a method of producing light varying in intensity in accordance With acoustic or the like oscillations which consists in applying separately to the electrodes of a glow discharge tube each of two sets of mutually independent electrical oscillations, one set of oscillations being of substantially constant amplitude and frequency and the other set of oscillations corresponding to the oscillations in accordance with which the light intensity is to be varied.
- a method of producing light varying in intensity in accordance with acoustic or the like oscillations which consists in applying separately to the electrodes of a glow discharge tube each of two sets of mutually independent electrical oscillations, one set of oscillations being of substantially constant amplitude and high frequency, and the other set of oscillations corresponding to the oscillations in accordance with Which the light intensity is to be varied.
- a method of producing light varying in intensity in accordance with acoustic or the like oscillations which consists in applying directly to the electrodes of a glow discharge tube electrical oscillations of substantially constant amplitude, and Simultaneously, but separately applying directly to 'said electrodes electrical oscillations corresponding to the oscillations in accordance'with which the light intensity is to be varied, but without substantially changing the amplitude of Said first-named oscillations.
- a method of producing light varying' in intensity in accordance with acoustic or the like oscillations which consists in applying directly to the electrodes of a glow discharge tube electrical oscillations of substantially constant amplitude, and simultaneously, but separately applying directly to said electrodes electrical oscillations corresponding to the oscillations in accordance With Which the light intensity is to be varied, said second named oscillations being applied to said electrodes in such a manner that the light emitted by one electrode of said glow discharge tube is, at substantially every instant, of different intensity than that emitted by another electrode.
- a method of producing light varying in intensity in accordance With acoustic or the like oscillations which consists in applying directly to the electrodes of a glow discharge tube electrical oscillations of substantially constant amplitude, and simultaneously, but separately applying directly to said electrodes electrical oscillations corresponding to the oscillations in accordance With which the light intensity is to be varied, said second named oscillations being applied to said electrodes in such a manner that the light emitted by one electrode of said glow discharge tube is, at substantially every instant, of diierent intensity than that emitted by another electrode, While the amplitude and frequency of the light wave representing the light emitted by said glow discharge tube as a whole remains a function of that emitted by each of said electrodes.
- the step which consists in applying directly to the electrodes of said tube electrical oscillations of constant amplitude and frequency and having a ripple wave length equal to the Width of said Slit.
- a device including a pair of electrodes, means for applying high frequency oscillations directly to said electrodes, and means for separately applying, also directly to said electrodes, oscillations of relatively lower frequency.
- a glow discharge device including a pair of electrodes, means for applying high frequency oscillations directly to said electrodes, and means independent of said first-named means for separately applying, also directly to said electrodes, oscillations of relatively lower frequency.
- a glow discharge de- Vice including a pair of electrodes, means for applying directly to said electrodes oscillations of substantially constant amplitude and frequency, and means independent of Said first named means for separately applying, also directly to said electrodes, oscillations of varying amplitude and frequency.
- a glow discharge device including a pair of electrodes, means for applying directly to said electrodes oscillations of substantially constant amplitude and frequency, and means independent of said first named means for separately applying, also directly to said electrodes, oscillations corresponding to the sound being recorded.
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Description
A. WHITAKER April 2, 1935.
PHOTOGRAPHIC RECORDING OF ACOUSTIC OR THE LIKE OSC ILLATIONS Filed June 11, 1929 Xd H U n U n U fl U n U U n HU n U n U n U n U n U H J 0 Ottomeys.
recording of such oscillations.
I by the gas in the region'of the two electrodes of be at earth potential and the instantaneous volt- Patented Apr. 2, 1935 v PHOTOGRAPHIC RECORDING OF ACOUSTIC I OR, THE LIKE OSCILLAT-IONS Alfred Whtaker, West Draytong England Signor, by mesne assgn ments, to Radio Corporation of America, New York, N. Y., a Corporation of Delaware l Application June 11, 1929, Serial No; 370,107
In Great Britain July 14, 1928 p y 11 Claims. (Cl. 179 -100.3)
electrode is at the higherpotential, The total light emitted by the tube is shown in Fig. 4; V
Fig. 5 illustrates the methOd-,accordingto the presentinventionin 'which the two oscillations of Figs. 1 and`2 arev added together. It will be no- UNITED STAT ENT 'O FICE The present invention relates, to the production ,of a light beam having an intensity which varies in accordance with acoustic OI' the like oscillations; more particularly for the photographic 'Where high frequency. electrical oscillation modulated With acoustic currents, are used to light a discharge tube the total light emitted by the tube, varies in accordance with the modulation, Since modulation of high frequency oscillations consists in varying, the amplitude of these oscillations in accordance with the acoustic currents. i
According to the present inventiona' glow discharge tube is employed andto the electrodes thereof are applied two sets of electrical oscillations, one set of oscillations being of substantially constant amplitude and frequency and the other set of oscillations corresponding to the oscillations in accordance with which the light intensity is to be varied. In this way,.the light emitted tained its constant amplitude but that, in effect, the center line OX in Fig. 1 has in Fig. 5 been deformed into 'the shape of the low frequency curve in Fig. 2. The light emitted by one electrode is a function of the shaded area above the line OX while that emitted by the other electrode is a function" of` the shaded area below the line OX. The intensity of the light emitted by the former electrode is indicated'by the plain dotted curve trode is .indicated by thechain dotted curve b. The total light emittedby the lamp is the sum of 'these twodotted curves and is represented by though the intensity of the light emitted by each ofthe electrodes -separately 'varies inaccordance with the low frequency oscillation in Fig; 2, that the tube, taken separately, is varied in accordan emitted' by the lamp as awhole is of much smaller with the oscillations to be recorded.
The invention Will be described with reference to the accompanying drawing in Which Figs. 1-6 are diagrams illustrating the method of the present invention in contrast With the known method using modulated high. frequency oscillations, and 4 Fig. 'lis a Circuit' dia the invention. y i
In the diagrams of' Figs.` 1 to Sand Fig.`5, one electrode of a glow discharge tube is assumed to plying the method of the present invention, therefore, the light from the two electrodesmust be .used simultaneously as` light Sources `provided that they are used to make separate records.
A suitable Circuit A for. carrying; the present, inventioninto effectis shown -in v Fig 7. High frequency oscillations are ed into the primary winding of thetransformer .d and the low frequency oscillations are fed intothe- 'primary winding `of :the transformer e. A condenser f serves to prevent lowfrequency oscillations from circulating in' the Circuit tothe left of the glow disch'arge 'tube g while a high frequency choke coil h prevents high frequency oscillations from circulating in the Circuit to the right of the discharge tube g.
The oscillations of constant frequency and amplitude have, preferably, a frequency above audibility but they may have an audible frequency to which the appara'tus is not sensitive. Where an optical slit is used for recording oscillations, it can be shown that when the ripple wave'length of the oscillations (that is to say' gram 'in accordance with age of the other electrode is plotted as ordinate, the line .OX representing Zero voltage and positive voltages being plotted in an upward direction. In Figs. 4 and 6, light intensity is plotted as ordinate, the axis OXrepreSenting Zero intensity. In all these diagrams, time is plotted as abscissa, the Scale being uniform in all the figures. The high frequency ripple is disregarded in Figs. 4 and 6.
Fig. 1 shows a high frequency oscillation of constant amplitude and Fig. 2 shows one complete period of a low frequency oscillation with which it is desired to modulate the intensity of the light emitted by the glow discharge tube. Fig. 3 illustrates the effect of modulating the oscillation of Fig. 1 by that of Fig. 2, the amplitude of the high frequency oscillation being varied in accordance with the low frequency oscillation. The total light emitted by the tube is a function of the total shaded area irrespective of which or shade upon the record) is equal to the'slit Width, no Variation in the light transmitted by the slit takes place. The apparatus, therefore, shows no response and is insensitive to the frequency corresponding to this wave length. In
the full lineficurve o. It will be seen that al- L amplitude' and of double the requency.` In apthe distance between successive bands of light r ticed that the high frequency oscillation has re-,
a. inFigG and that emitted by the other elecv be kept separate. v Bothelectrodes may, however;
some cases, therefore, oscillations of this frequency can be used in combination With the oscillations to be recorded as above described.
I claim:
1. A method of producing light varying in intensity in accordance With acoustic or the like oscillations Which consists in applying separately to the electrodes of a glow discharge tube each of two sets of mutually independent electrical oscillations, one set of oscillations being of substantially constant amplitude and frequency and the other set of oscillations corresponding to the oscillations in accordance with which the light intensity is to be varied.
2 A method according to claim l in Which said oscillations of constant amplitude and requency have a frequency above audibility.
3. A method of producing light varying in intensity in accordance with acoustic or the like oscillations which consists in applying separately to the electrodes of a glow discharge tube each of two sets of mutually independent electrical oscillations, one set of oscillations being of substantially constant amplitude and high frequency, and the other set of oscillations corresponding to the oscillations in accordance with Which the light intensity is to be varied.
4. A method of producing light varying in intensity in accordance with acoustic or the like oscillations which consists in applying directly to the electrodes of a glow discharge tube electrical oscillations of substantially constant amplitude, and Simultaneously, but separately applying directly to 'said electrodes electrical oscillations corresponding to the oscillations in accordance'with which the light intensity is to be varied, but without substantially changing the amplitude of Said first-named oscillations.
5. A method of producing light varying' in intensity in accordance with acoustic or the like oscillations which consists in applying directly to the electrodes of a glow discharge tube electrical oscillations of substantially constant amplitude, and simultaneously, but separately applying directly to said electrodes electrical oscillations corresponding to the oscillations in accordance With Which the light intensity is to be varied, said second named oscillations being applied to said electrodes in such a manner that the light emitted by one electrode of said glow discharge tube is, at substantially every instant, of different intensity than that emitted by another electrode. V
6. A method of producing light varying in intensity in accordance With acoustic or the like oscillations which consists in applying directly to the electrodes of a glow discharge tube electrical oscillations of substantially constant amplitude, and simultaneously, but separately applying directly to said electrodes electrical oscillations corresponding to the oscillations in accordance With which the light intensity is to be varied, said second named oscillations being applied to said electrodes in such a manner that the light emitted by one electrode of said glow discharge tube is, at substantially every instant, of diierent intensity than that emitted by another electrode, While the amplitude and frequency of the light wave representing the light emitted by said glow discharge tube as a whole remains a function of that emitted by each of said electrodes.
7. In the method of recording acoustic or the like oscillations photographically by means including a glow discharge tube and a light slit, the step Which consists in applying directly to the electrodes of said tube electrical oscillations of constant amplitude and frequency and having a ripple wave length equal to the Width of said Slit.
8. In a system for recording Sound by means of light, the combination of a glow discharge A device including a pair of electrodes, means for applying high frequency oscillations directly to said electrodes, and means for separately applying, also directly to said electrodes, oscillations of relatively lower frequency.
9. In a system for recording sound by means of light, the combination of a glow discharge device including a pair of electrodes, means for applying high frequency oscillations directly to said electrodes, and means independent of said first-named means for separately applying, also directly to said electrodes, oscillations of relatively lower frequency.
10. In a system for recording sound by means of light, the combination of a glow discharge de- Vice including a pair of electrodes, means for applying directly to said electrodes oscillations of substantially constant amplitude and frequency, and means independent of Said first named means for separately applying, also directly to said electrodes, oscillations of varying amplitude and frequency.
' 11. In a system for recording sound'by means of light, the combination of a glow discharge device including a pair of electrodes, means for applying directly to said electrodes oscillations of substantially constant amplitude and frequency, and means independent of said first named means for separately applying, also directly to said electrodes, oscillations corresponding to the sound being recorded.
ALFRED WI IITAKER.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB1996359X | 1928-07-14 |
Publications (1)
Publication Number | Publication Date |
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US1996359A true US1996359A (en) | 1935-04-02 |
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Application Number | Title | Priority Date | Filing Date |
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US370107A Expired - Lifetime US1996359A (en) | 1928-07-14 | 1929-06-11 | Photographic recording of acoustic or the like oscillations |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3233031A (en) * | 1960-06-27 | 1966-02-01 | Baldwin Co D H | Gating circuits for electrical musical instruments |
US3525900A (en) * | 1965-03-04 | 1970-08-25 | Microdot Inc | Frequency controlled enhancement of light emission |
-
1929
- 1929-06-11 US US370107A patent/US1996359A/en not_active Expired - Lifetime
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3233031A (en) * | 1960-06-27 | 1966-02-01 | Baldwin Co D H | Gating circuits for electrical musical instruments |
US3525900A (en) * | 1965-03-04 | 1970-08-25 | Microdot Inc | Frequency controlled enhancement of light emission |
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