US1314095A - Ckitstav beuthe - Google Patents

Ckitstav beuthe Download PDF

Info

Publication number
US1314095A
US1314095A US1314095DA US1314095A US 1314095 A US1314095 A US 1314095A US 1314095D A US1314095D A US 1314095DA US 1314095 A US1314095 A US 1314095A
Authority
US
United States
Prior art keywords
antenna
potential
circuit
node
point
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
Publication date
Application granted granted Critical
Publication of US1314095A publication Critical patent/US1314095A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q9/00Electrically-short antennas having dimensions not more than twice the operating wavelength and consisting of conductive active radiating elements
    • H01Q9/04Resonant antennas
    • H01Q9/30Resonant antennas with feed to end of elongated active element, e.g. unipole

Definitions

  • the potential node may be located at any point of the antenna between its upper an lower end, depending upon the manner in which the capacity and inductance is distributed.
  • control of the location of the potential'node may also be of great advantage in case'measuring instruments, signaling keys,
  • windings the distance between the iron core switches, spark gaps, or any other apparatus are used in the antenna circuit or adjacent circuits for which a potential against ground is highly undesirable.
  • the artificial control of the potential node in an antenna is however of particular value in case so-called frequency 'chan ers are used such as are, for instance, descri ed and illustrated in the patent to Arco-Meiss-- ner, Patent Number 1,181,556, atented May 2 1916.
  • frequency 'chan ers such as are, for instance, descri ed and illustrated in the patent to Arco-Meiss-- ner, Patent Number 1,181,556, atented May 2 1916.
  • the portion of e antenna which is used for coupling with the fre uency changer is oreover in such nd the winding must be made as short as evices which are frequentl re-- possible so as to avoid eddy currentsin the iron core which may otherwise be produced by stray fields.
  • the danger of flash-overs from the winding to the iron core in case of unduly high potentials is particularly great.
  • the primary winding of the apparatus and thedrest of the station may easily be dam: age
  • the conditions which afford the placing of the potential node into a certain point A of an antenna are that for both portions into which the antenna is divided by this point A, the product of the efi'ective capacity and the eflective self-induction which controls the oscillations at the time must have the same value and must be equal to the product of the' total effective capacity and self-induction of the entire radiation circuit. This condition can always be fulfilled.
  • b suitably distributing condensers and sel induction coils over the whole antenna.
  • Fi ure 1 shows the control of the potential no e in an antenna connected at its lower end to the counter-poise.
  • Fig. 2 shows the control of the potential node in an antennaconnected at its lower end to-ground;
  • Fig. 3 shows how two potential nodes may he produced in an antenna if desired.
  • Fig. 1, 1 is an antenna, 2 a coupling coil for couplin the antenna with any sultable primary osci lation circuit 3.
  • 4 is the counter-poise and 5 and 6 are two variable inductance'coils, one on each side of the coupling coil 2. It may be desirable to have the potential node of the antenna located at the point A. The sum of the self-inductances 5 and 6 is given by the required wave length. Now by suitably varying the inductances 5 and 6 relatively to each other, it is always possible to locate the potential node of the antenna at the point A. 4
  • 1 is the antenna, 2 a coupling coil which in this case may be conductively coupled with a suitable primary circuit 3.
  • the lower end' of the antenna is directly connected to 1 ground. It is again desired to place the potential node into the point A ofcoupling coil 2.
  • the inductance coils checking up the correct locatlon after the spark gap 9 of suitable size between point A p changer located therein and means for point has been determined, is to place a and the ground as shown in Fig. 2.
  • the ele- 1 ments 5, ,6 and 7 are varied until the spark .node in the antenna.
  • the other may be located in anotherv apparatus contained in the radiation circuit.
  • This modification is shown in Fig. 3.
  • r In this figure again 1 is the antenna, 4 the counter poise, and 10 the frequency changer of the character referred to above. 11 is an' ammeter. It is now desired to have one of potential nodes located'in the secondary of the changer 10 as at A and the other node I 8 and 12 are suitably dimensioned so that, the potential nodes are located at the points desired. It is of course obvious that for each given case the values of the condenser.

Landscapes

  • Transmitters (AREA)

Description

G; REUTHE. ANTENNA ARRANGEMENT FOR WIRELESS SIGNALING OR THE LIKE.
APPLICATION FILED MAY 25. I916.
Patented Aug. 26, 1919.
GUSTAV REU'IHE, OF SAYVILLE, NEW YORK.
ANTENNA ARRANGEMENT FOR WIRELESS SIGNALING OR THE LIKE.
Specification of Letters Patent.
Patented Aug. 26, 1919.
Application filed May 25, 1916. Serial No. 99,792.
' To all whom it may concern:
Be it known that I, GUSTAV REUTHE, a subject of the German Emperor, residing at Sayville, Long Island, New York, have invented certain new and useful Improvements in Antennae Arrangements for Wireless Signalin or the like, of which the following is a ull and clear specification.
In antennae for radiatin electric oscillations, which are connected inductively or conduc'tively with a primary circuit of any kind, the potential node may be located at any point of the antenna between its upper an lower end, depending upon the manner in which the capacity and inductance is distributed. 'I have found that it is of particular advantage to place the potential node of such antenna within that portion of it which is used for coupling. By this expedient above all the advantage is obtained, that between the antenna portion used for coupling and the primary circuit, or also between the primary circuit; and ground, only comparatively low potentials exist. Therefore all insulations which may be necessary at such portions of the oscillation circuits ma be made much lighter. Also protective d quired at such points in this kind 0 antenna can'be entirely dispensed with.
The control of the location of the potential'node may also be of great advantage in case'measuring instruments, signaling keys,
' wound on an iron core.'
windings the distance between the iron core switches, spark gaps, or any other apparatus are used in the antenna circuit or adjacent circuits for which a potential against ground is highly undesirable.
This expedient of suitably placing the potential node is important not only for the normal operation of a radio station but also I in case nearb .atmospheric discharges set up natural osci atlons 1n. the antenna. who
may be of very great amplitude.
The artificial control of the potential node in an antenna is however of particular value in case so-called frequency 'chan ers are used such as are, for instance, descri ed and illustrated in the patent to Arco-Meiss-- ner, Patent Number 1,181,556, atented May 2 1916. In an a paratus of t is character, the portion of e antenna which is used for coupling with the fre uency changer is oreover in such nd the winding must be made as short as evices which are frequentl re-- possible so as to avoid eddy currentsin the iron core which may otherwise be produced by stray fields. Thus in such instance the danger of flash-overs from the winding to the iron core in case of unduly high potentials is particularly great. In such case also the primary winding of the apparatus and thedrest of the station may easily be dam: age
The conditions which afford the placing of the potential node into a certain point A of an antenna are that for both portions into which the antenna is divided by this point A, the product of the efi'ective capacity and the eflective self-induction which controls the oscillations at the time must have the same value and must be equal to the product of the' total effective capacity and self-induction of the entire radiation circuit. This condition can always be fulfilled. b suitably distributing condensers and sel induction coils over the whole antenna.
simultaneously on both sides of the potential node.
In the accompanying drawings I have illustrated three modifications showing how my invention may be reduced to practice.
Of course these modifications are only typical, of the manner in which I propose to control the location of the potential node without limiting myself to 'the particular :forms shown. In these drawings Fi ure 1 shows the control of the potential no e in an antenna connected at its lower end to the counter-poise. Fig. 2 shows the control of the potential node in an antennaconnected at its lower end to-ground; and
Fig. 3 shows how two potential nodes may he produced in an antenna if desired.
Referring now to Fig. 1, 1 is an antenna, 2 a coupling coil for couplin the antenna with any sultable primary osci lation circuit 3. 4 is the counter-poise and 5 and 6 are two variable inductance'coils, one on each side of the coupling coil 2. It may be desirable to have the potential node of the antenna located at the point A. The sum of the self- inductances 5 and 6 is given by the required wave length. Now by suitably varying the inductances 5 and 6 relatively to each other, it is always possible to locate the potential node of the antenna at the point A. 4
Referring to Fig. 2, 1 is the antenna, 2 a coupling coil which in this case may be conductively coupled with a suitable primary circuit 3. In this modification the lower end' of the antenna is directly connected to 1 ground. It is again desired to place the potential node into the point A ofcoupling coil 2. For this purpose the inductance coils checking up the correct locatlon, after the spark gap 9 of suitable size between point A p changer located therein and means for point has been determined, is to place a and the ground as shown in Fig. 2. The ele- 1 ments 5, ,6 and 7 are varied until the spark .node in the antenna.
at gap 9 disappears. Of course any equivalent means for determining whether a potential exists between point A and the ground may be substituted for the spark {lnder certain circumstances it may be of advantagetohave more than one potential While one of these nodes may be located in the coupling coils,
the other may be located in anotherv apparatus contained in the radiation circuit. This modification is shown in Fig. 3. r In this figure again 1 is the antenna, 4 the counter poise, and 10 the frequency changer of the character referred to above. 11 is an' ammeter. It is now desired to have one of potential nodes located'in the secondary of the changer 10 as at A and the other node I 8 and 12 are suitably dimensioned so that, the potential nodes are located at the points desired. It is of course obvious that for each given case the values of the condenser.
and inductances which determine the locationof the node and of the wave length may be predetermined from the beginning without limiting the scope of my invention. Also it is obvious that in cases where only limited adjustments are required only one or the other of these elements (condensers or in ductances) may be made variable.
I claim:
1. The combination in a wireless signaling system of an antenna circuit, a'frequency said circuit into said frequency changer comprising a plurality of inductances and a capacity distributed over said circuit and proportioned relatively to. each other substantially as described.
2. The combination in a wireless signaling' system of an antenna circuit, an output circuit of a frequency changer connected therein and a plurality of inductances and a capacity distributed over said circuit and adapted for adjustment to different oscillatory frequencies to locate potential nodes at predetermined points in said antenna circuit.
GUSTAV REUTH-E.
US1314095D Ckitstav beuthe Expired - Lifetime US1314095A (en)

Publications (1)

Publication Number Publication Date
US1314095A true US1314095A (en) 1919-08-26

Family

ID=3381587

Family Applications (1)

Application Number Title Priority Date Filing Date
US1314095D Expired - Lifetime US1314095A (en) Ckitstav beuthe

Country Status (1)

Country Link
US (1) US1314095A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3259901A (en) * 1962-01-02 1966-07-05 Antenna Specialists Co Short half-wave antenna with plural loading coils
US3445849A (en) * 1966-02-14 1969-05-20 Rca Corp Half wavelength monopole antenna with spaced loading coils
US3656167A (en) * 1969-11-25 1972-04-11 Plessey Co Ltd Dipole radio antennae
US3680128A (en) * 1966-06-23 1972-07-25 Daphne Volkers Receiver with input phase control between antenna and chassis
US3909830A (en) * 1974-05-17 1975-09-30 Us Army Tactical high frequency antenna
DE2544345A1 (en) * 1974-10-04 1976-04-15 Thomson Csf WHOLE-WAVE VERTICAL ANTENNA
US4101898A (en) * 1976-07-26 1978-07-18 David Lee Ingram Base fed, top-loaded vertical whip antenna

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3259901A (en) * 1962-01-02 1966-07-05 Antenna Specialists Co Short half-wave antenna with plural loading coils
US3445849A (en) * 1966-02-14 1969-05-20 Rca Corp Half wavelength monopole antenna with spaced loading coils
US3680128A (en) * 1966-06-23 1972-07-25 Daphne Volkers Receiver with input phase control between antenna and chassis
US3656167A (en) * 1969-11-25 1972-04-11 Plessey Co Ltd Dipole radio antennae
US3909830A (en) * 1974-05-17 1975-09-30 Us Army Tactical high frequency antenna
DE2544345A1 (en) * 1974-10-04 1976-04-15 Thomson Csf WHOLE-WAVE VERTICAL ANTENNA
US4001833A (en) * 1974-10-04 1977-01-04 Thomson-Csf Whole wave vertical antenna
US4101898A (en) * 1976-07-26 1978-07-18 David Lee Ingram Base fed, top-loaded vertical whip antenna

Similar Documents

Publication Publication Date Title
US1314095A (en) Ckitstav beuthe
US2102410A (en) Antenna system
GB633397A (en) Improvements in automatic radio tuning systems
US2419577A (en) Antenna system
US2318361A (en) Loop assembly
GB571787A (en) Improvements in variable permeability tuning arrangements
US2452560A (en) Band-pass transformer
US2038294A (en) Coupling system
US2031016A (en) Method of and apparatus for testing electrical devices
US1316188A (en) Radiosignaling System
US2125119A (en) Coupling transformer
US2402260A (en) Permeability tuned short-wave spread-band receiver
US763893A (en) Wireless telegraphy.
US1512960A (en) Radio signaling system
US1156677A (en) Apparatus for the transmission of energy by electric oscillation.
US2568510A (en) Frequency divider
US1842916A (en) Static frequency changer
US1757333A (en) Frequency trap for radio signaling apparatus
US2117154A (en) All-wave antenna and coupler system
US1545523A (en) Means for transmitting time signals
US2707773A (en) Audio frequency transformer
US984762A (en) Apparatus for receiving electromagnetic waves.
US1407205A (en) Radio receiving- system
US2155838A (en) Direction finding system
US1829058A (en) High frequency transformer