US767997A - Space telegraphy. - Google Patents
Space telegraphy. Download PDFInfo
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- US767997A US767997A US19359204A US1904193592A US767997A US 767997 A US767997 A US 767997A US 19359204 A US19359204 A US 19359204A US 1904193592 A US1904193592 A US 1904193592A US 767997 A US767997 A US 767997A
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- 230000005499 meniscus Effects 0.000 description 36
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 34
- 229910052753 mercury Inorganic materials 0.000 description 34
- 239000007788 liquid Substances 0.000 description 24
- 229910000645 Hg alloy Inorganic materials 0.000 description 21
- 239000000463 material Substances 0.000 description 19
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 18
- 230000010355 oscillation Effects 0.000 description 17
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 16
- 229910052709 silver Inorganic materials 0.000 description 16
- 239000004332 silver Substances 0.000 description 16
- 238000000034 method Methods 0.000 description 15
- 239000002131 composite material Substances 0.000 description 14
- 239000004020 conductor Substances 0.000 description 10
- 238000004519 manufacturing process Methods 0.000 description 9
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 6
- 230000033001 locomotion Effects 0.000 description 6
- 230000015572 biosynthetic process Effects 0.000 description 5
- 229910052742 iron Inorganic materials 0.000 description 3
- 229910052697 platinum Inorganic materials 0.000 description 3
- 229910000497 Amalgam Inorganic materials 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 230000000994 depressogenic effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 239000010931 gold Substances 0.000 description 2
- 230000005484 gravity Effects 0.000 description 2
- 238000007654 immersion Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 230000003534 oscillatory effect Effects 0.000 description 2
- 230000001105 regulatory effect Effects 0.000 description 2
- IOVCWXUNBOPUCH-UHFFFAOYSA-N Nitrous acid Chemical compound ON=O IOVCWXUNBOPUCH-UHFFFAOYSA-N 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000011664 signaling Effects 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03D—DEMODULATION OR TRANSFERENCE OF MODULATION FROM ONE CARRIER TO ANOTHER
- H03D1/00—Demodulation of amplitude-modulated oscillations
- H03D1/14—Demodulation of amplitude-modulated oscillations by means of non-linear elements having more than two poles
- H03D1/18—Demodulation of amplitude-modulated oscillations by means of non-linear elements having more than two poles of semiconductor devices
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L27/00—Modulated-carrier systems
- H04L27/02—Amplitude-modulated carrier systems, e.g. using on-off keying; Single sideband or vestigial sideband modulation
- H04L27/06—Demodulator circuits; Receiver circuits
Definitions
- This invention relates to space or wireless I telegraphy by electromagnetic .waves in the form of electroradiant energy; and it relates' more particularly to methods of making electroreceptive devices which are adapted to utilize in their operation the dissipative energy of the electrical oscillations or oscillatory electric currents developed by electromagnetic waves in the circuits in which such devices are included.
- Electroreceptive devices of such character have long been known for detecting and measuring the energy of electromagnetic waves, and they are generally known as bolometers.
- serial N 0. 119,211, filed August 11, 1902 I have described the application of such electroreceptive devices to selective electric signaling and have therein claimed the same broadly.
- oscillatory electric currents developed in thereceiving-conductors of spacetelegraph systems are of small amplitude it is necessary to employ some means whereby the currents developed in the receiving system by electromagnetic waves may be amplified in order dissipated in the bolometer wire or strip without making the latter of excessively-high resistance.
- I For amplifying the currents developed in the receiving system by electromagnetic waves of a definite predetermined frequency I have described a resonant circuit or a group of resonant circuits attuned to such frequency.
- the resonant circuits strongly oppose the development therein of currents of frequencies difierent from that to which they are attuned, so that by means of such resonant circuits the bolometer fine wires or strips are protected from extraneous electrical forces which might otherwise destroy them.
- Figures 1 and 2 illustrate, respectively, the first and second stages in the formation of the bolometer herein described
- Fig. 3 represents thecompleted bolometer and its accessory apparatus connected in a space-telegraph receiving system.
- W represents a short length of Wire known as Wollaston Wire, greatly magnified.
- Dr. Wollaston Wire The method devised by Dr. Wollaston for producing this wire consists in incasing a fine platinum Wirein silver, reducing the composite wire so formed, and then 11y inventhat an appreciable amount of energy may be dissolying away the silver casing with warm nitrous acid.
- wireof diameteras small as one fifty-thousandth of an inch was produced, as fully set forth in the li'owyclopca' (Zia Britannica in anarticle entitled Wire, to which all those wishing to practice my invention are referred for further details concerning the manufacture of wire suitable for use in the bolometer herein described, although such wire has long been in commercial use and maybe obtained and, in fact, isusually obtained before the silver casing has been removed.
- a wire suitable for use in the bolometer herein described I recommend those sizes of Wollaston wire in which' the diameter of the inner wire is between .0001 inch and .00002 inch.
- the effect of the mercury or v the mercury alloy on the silver coating of the platinum wire is to form an amalgam ther'ewithv. 6., to dissolve the silver away from the platinum wirethus exposing the platinum wire from the upper end of the concave meniscus 4 in Fig. 1 to the lower end of the convex meniscus 4 in Fig. 2, formed by the mercury in contact with the platinum wire 2.
- mercury does not wet platinumz'. a, does not dissolve itso that its meniscus therewith is convex, as shown at L, Fig. 2, and it is also a fact that platinum has a greater specific gravity than mercury, so that the fine platinum wire is not forced out of the mercury.
- the length of the platinum wire from which the silver casing has beendissolved by the process above described, and which is thereby rendered effective as a bolometer fine wire is very short, indeed, be-
- VVollaston wire in this specification as a desirable means for obtaining the electrical conductor of small mass, yet I do not wish to confine myself to such specific means, because any wire or strip of small mass and of a metal irestrial vibration. which the bolometer fine wire or strip is conn'ected in the resonant circuit C 8 8 L I2. ;is a step-down transformer by which said not soluble in mercury or mercury alloy i. 6., not wetted by'the sameinca'sed' in a conductor soluble in'the mercury or mercury alloy z'.
- FIG. 3 is shown a practicable embodiment of this invention.
- H is a frame supporting an iron thimble 3 or other vessel of a material not soluble in mercury, containing mercury or an alloy or amalgam thereof, 3.
- 9 is a screw threaded into I the thimble 3, whereby the level of the mercury in the thimble may be elevated or depressed.
- 10 is a flat spring rigidly attached to the frame H at point 11 and bearing up wardly at its extreme end upon the flange of a micrometer-screw 12, threading into the base H", whereby the spring 10 may be depressed or elevated without lost motion. 6
- I7 is a stopper by The tube 6 is desirable to protect the bolometer-wire from ter- 8 8 are conductors by resonant circuit is associated with the ele-' vated conductor V.
- I1 and I2 are respectively the primary and'secondary windings of transformer M.
- R is a resistance
- B is a battery
- T is a signal-indicating device, preferably a telephone s receiver connected across the bolometer-wire
- L L are choking-coils connected between the bolometer and the signal-indicating device T.
- the length, and consequently the mass. of the platinum wire may be still further reduced by means of the micrometer-screw 12.
- the relative position of the screw 12 and the wire W with respect to the point of application of the-spring 10 to the frame H permits an exceedingly-fine adjustment of the length, and consequently the mass of the bolometer fine wire, as the movement of the wire may by these means be made any desired fraction of the translational movement of the screw.
- the micrometcrscrew may be operatively connected with the vessel containing the mercury, so that the adjustment of the mass of the bolometer fine wire or strip may be made without moving the wire or strip, but by moving the mercury with respect to said wire or strip.
- VVhile I have herein specifically referred to the screw 12 as a micrometer-screw, I desire to be understood as meaning thereby any screw of small pitch, whereby a considerable rotational movement is required to produce an appreciable translational movement.
- ⁇ Vhile I have de' scribed a particular form of spring for overcoming the lost motion of the screw 12, it will be understood thatthis form is merely one of many. forms of spring which will accomplish this result.
- I claim 1 The method of making a bolometer wire or strip of small mass which consists in immersing the lower end of a length of platinum wire ineased in silver in a bath of mercury or mercury alloy, thereby causing the mercury or mercury alloy to form a concave meniscus with the silver casing, dissolving away that part ofthe silver casing which is wettcd by the mercury or mercury alloy until the mercury or mercury alloy forms a convex meniscus with the inner platinum wire, and thereby exposing a length of platinum wire equal approximately to the sum of the lengths of the concave meniscus and the convex meniscus.
- a bolometer comprising a wire or strip of small mass which consists in immersing in a bath of mercury or mercury alloy, the lower end of a length of wire or strip of a material not soluble in mercury or mercury alloy and incased in a material which is soluble in mercury or mercury alloy, thereby causing the mercury or mercury alloy to form, first, a concave meniscus with the material of the-casing, and second, a convex meniscus with the inner wire, thereby dissolving away a portion of the material of the casing equal approximately in length to the sum of the lengths of. the concave meniscus and the convex miniscus, and finally immersing the resulting fine wire or strip still further in the mercury or mercury alloy, or partially withdrawing it therefrom.
- a bolometer comprising a fine wire or strip of small mass adapted for use as a receiver for space-telegraph signals
- the method of producing an adjustable bolometer wire or strip which consists in immersing one end of such wire or strip in a conducting liquid and varying the extent of such immersion.
- the method of producing an adjustable bolometer wire or strip which consists in immersing one end of such wire or strip in a conducting liquid and varying the extent of such immersion.
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Radiation-Therapy Devices (AREA)
Description
\A/ITIJ EEEEI INJ N d m. ,4; Mad All? No. 767,997. I PATENTED AUG. 16, 1904;
J. S. STONE.
SPACE TELEGRAPHY.
APPLICATION FILED FEB. 15. 190 1.
N0 MODEL aLD NW UNITED STATES Patented August 16, 1904.
PATENT OFFICE;
JOHN STONE STONE, OF CAMBRIDGE, MASSAOHUSETTS, ASSIGNOR TO INILLIALI W. SWAN, TRUSTEE, OF BROOKLINE, lVIASSACI-IUSETTS.
SPACE TELEGRAPHY.
SPECIFICATION forming part of Letters Patent N0. 767,997, dated August 16, 1904.
Application filed February 15,1904. SerialNo. 193,592.
State'of lW-assachusetts, have invented cernain new and useful Improvements in Space 'elegraphy, of which the following is a specification. I
This invention relates to space or wireless I telegraphy by electromagnetic .waves in the form of electroradiant energy; and it relates' more particularly to methods of making electroreceptive devices which are adapted to utilize in their operation the dissipative energy of the electrical oscillations or oscillatory electric currents developed by electromagnetic waves in the circuits in which such devices are included. Electroreceptive devices of such character have long been known for detecting and measuring the energy of electromagnetic waves, and they are generally known as bolometers. In my application Serial N 0. 119,211, filed August 11, 1902, I have described the application of such electroreceptive devices to selective electric signaling and have therein claimed the same broadly. In my application Serial No. 182,628, filed November 25, 1903, I have described and claimed a specific form-of such electroreceptive device and a particular form of space-telegraph receiv ing system in which the same may be employed. In said applications I have pointed out that in order to be rapidly responsive to changes in thermal conditionz'. a, in order to be sensitive-the fine wires or strips of such bolometers should be of small thermal time constant compared to the thermal time constants of the bolometers heretofore used for experimental purposes, and that in order to be of such small thermal time constant the fine wires or strips should be of small mass 2'. e. of small length and small sectionshould be of a material of low specific heat and that the heat insulation of the fine wires or strips should not be too perfect. I have also pointed out that for greater efficiency the bolometer fine wires or strips should be of high-resistance temperature coefficient and of high specific resistance. I have also shown that as the (N0 model.)
! oscillatory electric currents developed in thereceiving-conductors of spacetelegraph systems are of small amplitude it is necessary to employ some means whereby the currents developed in the receiving system by electromagnetic waves may be amplified in order dissipated in the bolometer wire or strip without making the latter of excessively-high resistance. For amplifying the currents developed in the receiving system by electromagnetic waves of a definite predetermined frequency I have described a resonant circuit or a group of resonant circuits attuned to such frequency. The resonant circuits strongly oppose the development therein of currents of frequencies difierent from that to which they are attuned, so that by means of such resonant circuits the bolometer fine wires or strips are protected from extraneous electrical forces which might otherwise destroy them.
The present invention mayibe best understood by having reference to the drawings which accompany and form a part of this specification and which illustrate an apparatus whereby the herein described method of making an electric receptive device adapted for use. in receiving space-telegraph signals may be conveniently carried out'. tion, however, is broader than mere apparatus and is capable of being carried into effect in a variety of ways, while the particular apparatus herein illustrated forms no part of the present invention, having been claimed in my application Serial No. 193,591, filed simultaneously herewith.
In the drawings, Figures 1 and 2 illustrate, respectively, the first and second stages in the formation of the bolometer herein described, and Fig. 3 represents thecompleted bolometer and its accessory apparatus connected in a space-telegraph receiving system.
. In the figures, W represents a short length of Wire known as Wollaston Wire, greatly magnified. The method devised by Dr. Wollaston for producing this wire consists in incasing a fine platinum Wirein silver, reducing the composite wire so formed, and then 11y inventhat an appreciable amount of energy may be dissolying away the silver casing with warm nitrous acid. In this way wireof diameteras small as one fifty-thousandth of an inch was produced, as fully set forth in the li'owyclopca' (Zia Britannica in anarticle entitled Wire, to which all those wishing to practice my invention are referred for further details concerning the manufacture of wire suitable for use in the bolometer herein described, although such wire has long been in commercial use and maybe obtained and, in fact, isusually obtained before the silver casing has been removed. As a wire suitable for use in the bolometer herein described I recommend those sizes of Wollaston wire in which' the diameter of the inner wire is between .0001 inch and .00002 inch.
The method of giving to the platinum wire, which forms the fine wire of the bolometer herein'described, the requisite short length, and consequently the desired. small mass, in
. virtue of which the temperature of such fine wire may be appreciably elevated by small amounts of energy, is'as follows: The VVollaston wire is immersed to any desired depth in a bath of mercury or mercury alloy 3, con- 'tained in a vessel 3, such as an iron thimble. Inasmuch as mercury wets silver the meniscus formed with the silver coating 1 of the platinum wire 2 is concave, as shown at 4:. This, as is well understoodpis caused by capillary attraction and by the adhesion of the mercury to the silver. When mercury does not wet a metald. e. when the metalis not soluble in melrcury the meniscus is convex; as shown at 5, where the mercury contacts the walls of the iron thimble. The effect of the mercury or v the mercury alloy on the silver coating of the platinum wire is to form an amalgam ther'ewithv. 6., to dissolve the silver away from the platinum wirethus exposing the platinum wire from the upper end of the concave meniscus 4 in Fig. 1 to the lower end of the convex meniscus 4 in Fig. 2, formed by the mercury in contact with the platinum wire 2. It is a fact that mercury does not wet platinumz'. a, does not dissolve itso that its meniscus therewith is convex, as shown at L, Fig. 2, and it is also a fact that platinum has a greater specific gravity than mercury, so that the fine platinum wire is not forced out of the mercury. The length of the platinum wire from which the silver casing has beendissolved by the process above described, and which is thereby rendered effective as a bolometer fine wire, is very short, indeed, be-
ing, in fact, equal approximately to the sum of the lengths of the concave meniscus 4 and the convex meniscus 4.
Although I have specially referred to VVollaston wire in this specification as a desirable means for obtaining the electrical conductor of small mass, yet I do not wish to confine myself to such specific means, because any wire or strip of small mass and of a metal irestrial vibration. which the bolometer fine wire or strip is conn'ected in the resonant circuit C 8 8 L I2. ;is a step-down transformer by which said not soluble in mercury or mercury alloy i. 6., not wetted by'the sameinca'sed' in a conductor soluble in'the mercury or mercury alloy z'. a, wetted by the samecan be substituted for the Wollaston wire, provided the specific gravity of the incased conductor be 1 such that it will not be forced out of the mercury or mercury alloy. Gold possesses these characteristics, and therefore a composite wire formed of gold incased in silver or other ductile metal soluble in mercury or mercury alloy may be employed.
In Fig. 3 is shown a practicable embodiment of this invention. In this figure, H is a frame supporting an iron thimble 3 or other vessel of a material not soluble in mercury, containing mercury or an alloy or amalgam thereof, 3. 9 is a screw threaded into I the thimble 3, whereby the level of the mercury in the thimble may be elevated or depressed. 10 is a flat spring rigidly attached to the frame H at point 11 and bearing up wardly at its extreme end upon the flange of a micrometer-screw 12, threading into the base H", whereby the spring 10 may be depressed or elevated without lost motion. 6
is a glass tube rigidly attached to the spring 10 and containing a-length of Wollaston wire -.W in its silver jacket; which the VVollaston wire is sealed into the upper end of the tube.
7 is a stopper by The tube 6 is desirable to protect the bolometer-wire from ter- 8 8 are conductors by resonant circuit is associated with the ele-' vated conductor V. I1 and I2 are respectively the primary and'secondary windings of transformer M. R is a resistance, B is a battery, and T is a signal-indicating device, preferably a telephone s receiver connected across the bolometer-wire, and L L are choking-coils connected between the bolometer and the signal-indicating device T.
After the silver casing has been dissolved from the platinum wire, as above described, the length, and consequently the mass. of the platinum wire may be still further reduced by means of the micrometer-screw 12. The relative position of the screw 12 and the wire W with respect to the point of application of the-spring 10 to the frame H permits an exceedingly-fine adjustment of the length, and consequently the mass of the bolometer fine wire, as the movement of the wire may by these means be made any desired fraction of the translational movement of the screw. I do not wish to be limited to the form of apparatus herein described, as it is obvious that many changes may be made therein without departing from the spirit of my invention. For example, the micrometcrscrew may be operatively connected with the vessel containing the mercury, so that the adjustment of the mass of the bolometer fine wire or strip may be made without moving the wire or strip, but by moving the mercury with respect to said wire or strip. VVhile I have herein specifically referred to the screw 12 as a micrometer-screw, I desire to be understood as meaning thereby any screw of small pitch, whereby a considerable rotational movement is required to produce an appreciable translational movement. \Vhile I have de' scribed a particular form of spring for overcoming the lost motion of the screw 12, it will be understood thatthis form is merely one of many. forms of spring which will accomplish this result.
I claim 1. The method of making a bolometer wire or strip of small mass which consists in immersing the lower end of a length of platinum wire ineased in silver in a bath of mercury or mercury alloy, thereby causing the mercury or mercury alloy to form a concave meniscus with the silver casing, dissolving away that part ofthe silver casing which is wettcd by the mercury or mercury alloy until the mercury or mercury alloy forms a convex meniscus with the inner platinum wire, and thereby exposing a length of platinum wire equal approximately to the sum of the lengths of the concave meniscus and the convex meniscus.
2. The method of making a bolometer wire or strip of small mass which consists in immersing in a bath of mercury or mercury alloy, the lower end of alength of wire or strip of a material not soluble in mercury or mercury alloy and incased in a material which is soluble in mercury or mercury alloy, thereby causing the mercury or mercury alloy toform, first, a concave meniscus with the material of the casing, and second, a convex meniscus with the inner wire, and thereby dissolving away a portion of the material of the casing equal approximately in length to the sum of the lengths of the concave meniscus and the convex meniscus.
3. The method of making a bolometer comprising a wire or strip of small mass which consists in immersing in a bath of mercury or mercury alloy, the lower end of a length of wire or strip of a material not soluble in mercury or mercury alloy and incased in a material which is soluble in mercury or mercury alloy, thereby causing the mercury or mercury alloy to form, first, a concave meniscus with the material of the-casing, and second, a convex meniscus with the inner wire, thereby dissolving away a portion of the material of the casing equal approximately in length to the sum of the lengths of. the concave meniscus and the convex miniscus, and finally immersing the resulting fine wire or strip still further in the mercury or mercury alloy, or partially withdrawing it therefrom.
4. As an improvement in the art of making a bolometer comprising a fine wire or strip of small mass adapted for use as a receiver for space-telegraph signals, the method herein described of dissolving away the desired amount of the silver casing of a Vollaston wire by means of mercury or an alloy of mercury.
5. As an improvement in the art of making a bolometer comprising a fine wire or strip of small mass adapted for use as a receiver for space-telegraph signals, the method herein described of dissolving away the desired amount of the outer casing of a composite wire by immersing the composite wire in a conducting liquid in which the inner wire is insoluble and then adjusting the length of the resulting wire by still further immersing it in said conducting liquid, or partially withdrawing it therefrom.
6. As an improvement in the art of making an electroreceptive device for space-telegraph signals adapted to utilize in its operation the dissipative energy of the electrical oscillations developed by electromagnetic waves in a receiving system, the method herein described of immersing in a conductingliquid a wire or strip of amaterial insoluble in said liquid and incased in a material which is soluble in said liquid, thereby dissolving away a portion of the outer casing of said wire or strip, and finally regulating the length of said wire or strip thereby exposed from said outer casin 7 As an improvement in the art of making an electroreceptive device for space-telegraph signals adapted to utilize in its operation the dissipative energy of the electrical oscillations developed by electromagnetic waves in a receiving system, the method herein described of dissolving away the desired amount of the outer casing of a composite wire by means of mercury or an alloy of mercury.
8. As an improvement in the art of making an electroreceptive device for space-telegraph signals adapted to utilize in its operation the dissipative energy of the electrical oscillations developed by electromagnetic waves in a receiving system, the method herein described of dissolving away the desired amount of the outer casing of a composite Wire by immersing said composite wire in a conducting liquid in which the outer casing of said composite wire is soluble and regulating the length of the inner wire thereby exposed from said outer casing by means of a micrometer-screw.
9. The method of receiving space-telegraph signals which consists in absorbing the energy of electromagnetic signal-waves by an elevated conductor, thereby creating electrical oscillations in said elevated conductor, conveying said electrical oscillations at increased current to a resonant circuit attuned to the frequency of the waves the energy of which is to be received, amplifying said electrical oscillations by means of said resonant circuit, and utilizing the dissipative energy of the electrical oscillations so amplified by said reso- 1 l i i i nant circuit to vary the normal temperature, and thereby the dissipative resistance, of an electroreceptive device comprising a fine wire or strip immersed in a conducting liquid.
5 10. The method of receiving space-telegraph signals which consists in absorbing the energy of electromagnetic signal-waves by an elevated conductor, thereby creating elec trical oscillations in said elei'ated conductor,
10 conveying said electrical oscillations to a resonant circuit attuned to the frequency of the waves the energy. of which is to be received, amplifying said electrical oscillations by means of said resonant circuit, and utilizing I5 the dissipative energy of the electrical oscillations so amplified by said resonant circuit to vary the normal temperature, and thereby the dissipative resistance, of an electroreceptive device comprising a fine Wire or strip im- 2 mersed in a conducting liquid.
11. The method of producing intelligible signals transmitted by electromagnetic sig- -nal-waves which consists in amplifying the electrical oscillations resulting from said elec- 5 tromagnetic signal-waves by means of a cir- 3 pative resistance of an electroreceptive device comprising a fine wire or strip immersed in a conducting liquid.
12. The method of making a bolometer fine Wire or strip of small mass, which consists in 35 immersing the lower end of a length of wire or strip of one material incased in a casing of a different material in a bath of conducting liquid in which said wire or strip is insoluble [snare] and in which said casing is soluble and which will form a concave meniscus with the material of the casing and a convex meniscus with the material of the wire or strip, thereby causing the formation successively of a concave meniscus between the liquid and the easing and a convex meniscus between the liquid and the inner wire or strip, and thereby ex posing from said casing a length of the inner wire or strip equal approximately to the sum of the lengths of the concave meniscus and the convex meniscus.
13. The method of making a bolometer wire or strip of small mass, which consists in immersing the lower end of a length of composite wire in a bath of conducting liquid, thereby causing the successive formation of a concave meniscus between the liquid and the easing and a convex meniscus between the liquid and the inner wire of said composite wire, and thereby exposing from the outer casing of the composite wire a length of the inner wire equal approximately to the sum of the lengths of the concave meniscus and the convex menisone.
1%. The method of producing an adjustable bolometer wire or strip, which consists in immersing one end of such wire or strip in a conducting liquid and varying the extent of such immersion.
In testimony whereof I have hereunto subscribed my name this llth day of February, 1904.
JOHN STONE STONE.
Witnesses:
BRAINERD T. JUDKINs, (Jr. ADELAIDE HIGGINs.
It is hereby certified that in Letters Patent No. 767,997, granted August 16, 1904, upon the application of John Stone Stone, Cambridge, Massachusetts, for an improvement in Space Telegraphy, errors appear in the printed specification requiring correction, as follows: On page 2, line 56, the comma after the word short should be stricken out; in line 107, a comma should be inserted after the word receiver; and i in line 120, a coinma should be inserted after the Word mass; and-that the said Letters Patent should be read with these corrections therein that the same may conform to the record of the case in the Patent Ofiice.
Signed and sealed this 4th day of July, A. D., 1905.
F. I. ALLEN,
Commissioner of Patents.
1 l i i i nant circuit to vary the normal temperature, and thereby the dissipative resistance, of an electroreceptive device comprising a fine wire or strip immersed in a conducting liquid.
5 10. The method of receiving space-telegraph signals which consists in absorbing the energy of electromagnetic signal-waves by an elevated conductor, thereby creating elec trical oscillations in said elei'ated conductor,
10 conveying said electrical oscillations to a resonant circuit attuned to the frequency of the waves the energy. of which is to be received, amplifying said electrical oscillations by means of said resonant circuit, and utilizing I5 the dissipative energy of the electrical oscillations so amplified by said resonant circuit to vary the normal temperature, and thereby the dissipative resistance, of an electroreceptive device comprising a fine Wire or strip im- 2 mersed in a conducting liquid.
11. The method of producing intelligible signals transmitted by electromagnetic sig- -nal-waves which consists in amplifying the electrical oscillations resulting from said elec- 5 tromagnetic signal-waves by means of a cir- 3 pative resistance of an electroreceptive device comprising a fine wire or strip immersed in a conducting liquid.
12. The method of making a bolometer fine Wire or strip of small mass, which consists in 35 immersing the lower end of a length of wire or strip of one material incased in a casing of a different material in a bath of conducting liquid in which said wire or strip is insoluble [snare] and in which said casing is soluble and which will form a concave meniscus with the material of the casing and a convex meniscus with the material of the wire or strip, thereby causing the formation successively of a concave meniscus between the liquid and the easing and a convex meniscus between the liquid and the inner wire or strip, and thereby ex posing from said casing a length of the inner wire or strip equal approximately to the sum of the lengths of the concave meniscus and the convex meniscus.
13. The method of making a bolometer wire or strip of small mass, which consists in immersing the lower end of a length of composite wire in a bath of conducting liquid, thereby causing the successive formation of a concave meniscus between the liquid and the easing and a convex meniscus between the liquid and the inner wire of said composite wire, and thereby exposing from the outer casing of the composite wire a length of the inner wire equal approximately to the sum of the lengths of the concave meniscus and the convex menisone.
1%. The method of producing an adjustable bolometer wire or strip, which consists in immersing one end of such wire or strip in a conducting liquid and varying the extent of such immersion.
In testimony whereof I have hereunto subscribed my name this llth day of February, 1904.
JOHN STONE STONE.
Witnesses:
BRAINERD T. JUDKINs, (Jr. ADELAIDE HIGGINs.
It is hereby certified that in Letters Patent No. 767,997, granted August 16, 1904, upon the application of John Stone Stone, Cambridge, Massachusetts, for an improvement in Space Telegraphy, errors appear in the printed specification requiring correction, as follows: On page 2, line 56, the comma after the word short should be stricken out; in line 107, a comma should be inserted after the word receiver; and i in line 120, a coinma should be inserted after the Word mass; and-that the said Letters Patent should be read with these corrections therein that the same may conform to the record of the case in the Patent Ofiice.
Signed and sealed this 4th day of July, A. D., 1905.
F. I. ALLEN,
Commissioner of Patents.
ions in Letters Patent No. 767,997.
Correct It is hereby certified that in Letters Patent No. 767,997, granted August 16, 1904, upon the application of John Stone Stone, Cambridge, Massachusetts, for an improvement in Space Telegraphy, errors appear in the printed specification requiring correction, as follows: On page 2, line 56, the comma after the word short should be stricken out; in line 107, a comma should be inserted after the word receiver; and in line 120, a comma should be inserted after the word mass; and that the said Letters Patent should he read with these corrections therein that the same may conform to the record of the case in the Patent Oflice.
Signed and sealed this 4th day of July, A. D., 1905.
[snub] F. I. ALLEN,
Commissioner of Patents.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US19359204A US767997A (en) | 1904-02-15 | 1904-02-15 | Space telegraphy. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US19359204A US767997A (en) | 1904-02-15 | 1904-02-15 | Space telegraphy. |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US767997A true US767997A (en) | 1904-08-16 |
Family
ID=2836483
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US19359204A Expired - Lifetime US767997A (en) | 1904-02-15 | 1904-02-15 | Space telegraphy. |
Country Status (1)
| Country | Link |
|---|---|
| US (1) | US767997A (en) |
-
1904
- 1904-02-15 US US19359204A patent/US767997A/en not_active Expired - Lifetime
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