US2375593A - Reception of signals on a loop antenna - Google Patents

Reception of signals on a loop antenna Download PDF

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Publication number
US2375593A
US2375593A US481406A US48140643A US2375593A US 2375593 A US2375593 A US 2375593A US 481406 A US481406 A US 481406A US 48140643 A US48140643 A US 48140643A US 2375593 A US2375593 A US 2375593A
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Prior art keywords
loop
core
inductance
reception
loop antenna
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Expired - Lifetime
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US481406A
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Carl G Sontheimer
Robett S Doak
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RCA Corp
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RCA Corp
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Priority to US481406A priority Critical patent/US2375593A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q7/00Loop antennas with a substantially uniform current distribution around the loop and having a directional radiation pattern in a plane perpendicular to the plane of the loop
    • H01Q7/06Loop antennas with a substantially uniform current distribution around the loop and having a directional radiation pattern in a plane perpendicular to the plane of the loop with core of ferromagnetic material

Definitions

  • This invention relates to 100p antennas, and more particularly to a method of and means for providing increased signal pickup for a given loop inductance.
  • the figure of merit of a loop antenna for use with radio receivers, direction finders, and the like is the ratio of effective height to the square root of the loop inductance.
  • the effective height of a loop represents the factor which, when multiplied by the field strength in microvolts per meter, gives a measure of the E. M. F. generated in the loop.
  • the inductance, L, of a loop antenna is approximately proportional to WA.
  • both the effective height and the square root of the inductance are substantially proportional to the number of turns, and
  • the figure of merit, h/ L is substantially independent of the number of turns on the loop.
  • the power extracted from a radiation field by a loop depends basically on the radiation resistance of the loop; but this effect is ordinarily masked by the inductance of the loop.
  • the principal object of the present invention is to provide an improved loop construction and method whereby the advantages of increased effective height may beobtained without corresponding increase in the inductance.
  • a further object is to provide loop antennas having a greater ratio of effective height to the square root of inductance than prior loop antennas.
  • Fig. 1 illustrates the construction of one embodiment of the invention
  • Fig. 2 shows a modified construction.
  • a closed core I of magnetically permeable material such as comminuted iron oxide, powdered iron mixed with a suitable binder material, or the like, is provided with a winding comprising coils 3 and 5 disposed on the legs 1 and 9 respectively of the core I.
  • the coils are connected in series in reverse polarities to each other between terminal II and I3, so that the mutual inductance between the two legs of the winding is such as to diminish the net series inductance.
  • the arrows Hs on the drawing represent the magnetic flux of a radiation field linking the coils 3 and 5.
  • the voltages 8s induced in the two coils are additive, i. e. the output voltage of the loop is substantially twice that of either coil.
  • the series inductance of the two coils is:
  • L1 and L2 are the self inductances of the coils 3 and 5 respectively, and K is the coefiicient of coupling between them. If the permeability of the core I were infinite, L would be zero, and the total voltage would still be the sum of the voltages induced in the two coils.
  • the expression 2K ⁇ /L1 L2 represents the mutual inductance which is opposed to either of the self inductances. The effectiveness of loops constructed in accordance with the invention is thus largely dependent upon the permeability of the core material.
  • a core iii of toroidal shape is employed.
  • the windings are disposed on this core in a manner similar to the arrangement of the windings 3 and 5 on the core of Fig. l.
  • the operation of this structure is identical with that of the loop of Fig. 1. It should be apparent without further illustration that either of the windings may be wound in a reverse direction, provided the connections thereto are interchanged.
  • the invention has been described as an improved loop antenna structure, comprising spaced coils coupled together by means of a closed magnetic core to provide mutual inductance which is opposed to the self inductances of the spaced coils.
  • This arrangement provides an improvement in the ratio of effective height to inductance over prior artstructures.
  • a directive antenna comprising a closed core of magnetically permeable material, and windings disposed on spaced axes on said core and connected in series with each other in such relationship that the mutual inductance between said windings is opposed to the self inductances thereof.
  • a directive antenna comprising a closed core of magnetically permeable material, and windings disposed on spaced parallel axes on said core and connected in series with each other in such relationship that the mutual inductance between said windings is opposed to the self inductances thereof.
  • a directive antenna comprising a substantially toroidal core of magnetically permeable material, and windings disposed on spaced arcs on said core and connected in series with each other in such relationship that the mutual inductance between said windings is opposed to the self inductances thereof.

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Description

y 1945- c. G. SONTHEIMER ET AL 2,375,593
RECEPTION OF SIGNALS ON A LOOP ANTENNA Filed April 1, 1945 Isnnentors 68 M Gttorneg Patented May 8, 1945 RECEPTION OF SIGNALS ON A LOOP ANTENNA Carl G. Sontheimer, Haddonfield, and Robert S. Doak, Collingswood, N. J., assignors to Radio Corporation of America, a corporation of Dela- Application April 1, 1943, Serial No. 481,406
3 Claims. (01. 250-33) This invention relates to 100p antennas, and more particularly to a method of and means for providing increased signal pickup for a given loop inductance. The figure of merit of a loop antenna for use with radio receivers, direction finders, and the like, is the ratio of effective height to the square root of the loop inductance. The effective height of a loop represents the factor which, when multiplied by the field strength in microvolts per meter, gives a measure of the E. M. F. generated in the loop. The effective height, h=21r7 A/ meters, where n=number of turns, and A=area of each turn in square meters.
The inductance, L, of a loop antenna is approximately proportional to WA. Thus for a loop of given area, both the effective height and the square root of the inductance are substantially proportional to the number of turns, and
the figure of merit, h/ L, is substantially independent of the number of turns on the loop. The power extracted from a radiation field by a loop depends basically on the radiation resistance of the loop; but this effect is ordinarily masked by the inductance of the loop.
The principal object of the present invention is to provide an improved loop construction and method whereby the advantages of increased effective height may beobtained without corresponding increase in the inductance.
A further object is to provide loop antennas having a greater ratio of effective height to the square root of inductance than prior loop antennas. g E
Referring to the drawing, Fig. 1 illustrates the construction of one embodiment of the invention, and Fig. 2 shows a modified construction.
A closed core I, of magnetically permeable material such as comminuted iron oxide, powdered iron mixed with a suitable binder material, or the like, is provided with a winding comprising coils 3 and 5 disposed on the legs 1 and 9 respectively of the core I. The coils are connected in series in reverse polarities to each other between terminal II and I3, so that the mutual inductance between the two legs of the winding is such as to diminish the net series inductance.
The arrows Hs on the drawing represent the magnetic flux of a radiation field linking the coils 3 and 5. The voltages 8s induced in the two coils are additive, i. e. the output voltage of the loop is substantially twice that of either coil.
The series inductance of the two coils is:
=L1+L22K\/Ll L2 where L1 and L2 are the self inductances of the coils 3 and 5 respectively, and K is the coefiicient of coupling between them. If the permeability of the core I were infinite, L would be zero, and the total voltage would still be the sum of the voltages induced in the two coils. The expression 2K\/L1 L2 represents the mutual inductance which is opposed to either of the self inductances. The effectiveness of loops constructed in accordance with the invention is thus largely dependent upon the permeability of the core material.
Referring to Fig. 2, a core iii of toroidal shape is employed. The windings are disposed on this core in a manner similar to the arrangement of the windings 3 and 5 on the core of Fig. l. The operation of this structure is identical with that of the loop of Fig. 1. It should be apparent without further illustration that either of the windings may be wound in a reverse direction, provided the connections thereto are interchanged.
Thus the invention has been described as an improved loop antenna structure, comprising spaced coils coupled together by means of a closed magnetic core to provide mutual inductance which is opposed to the self inductances of the spaced coils. This arrangement provides an improvement in the ratio of effective height to inductance over prior artstructures.
We claim as our invention:
1. A directive antenna comprising a closed core of magnetically permeable material, and windings disposed on spaced axes on said core and connected in series with each other in such relationship that the mutual inductance between said windings is opposed to the self inductances thereof.
2. A directive antenna comprising a closed core of magnetically permeable material, and windings disposed on spaced parallel axes on said core and connected in series with each other in such relationship that the mutual inductance between said windings is opposed to the self inductances thereof.
3. A directive antenna comprising a substantially toroidal core of magnetically permeable material, and windings disposed on spaced arcs on said core and connected in series with each other in such relationship that the mutual inductance between said windings is opposed to the self inductances thereof.
CARL G. SON'I'HEIMER. ROBERT S. DOAK.
US481406A 1943-04-01 1943-04-01 Reception of signals on a loop antenna Expired - Lifetime US2375593A (en)

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Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2975421A (en) * 1956-02-28 1961-03-14 George D Chichester Magnetic antenna
US2996717A (en) * 1959-02-06 1961-08-15 Hazeltine Research Inc Wave focusing antenna
US3066292A (en) * 1954-10-05 1962-11-27 Casco Products Corp Automoble antenna with toroid coil and magnetic core
US3353132A (en) * 1965-05-27 1967-11-14 Gen Electric Leakage flux suppressor windings for transformers
US3495264A (en) * 1966-12-09 1970-02-10 Continental Electronics Mfg Loop antenna comprising plural helical coils on closed magnetic core
FR2608845A1 (en) * 1986-12-22 1988-06-24 Pizon Ernest Receiving or transmitting antenna esp. for car radio - has prim. winding of coupling transformer inserted into loop formed by windings on rectangular ferrite bars
US5023585A (en) * 1988-11-17 1991-06-11 Murata Manufacturing Co., Ltd. Common-mode choking coil
US20030132889A1 (en) * 2002-01-04 2003-07-17 Darfon Electronics Copr. Loop antenna
US20150207232A1 (en) * 2014-01-20 2015-07-23 Raytheon Company High efficiency polarized ulf/vlf/rf transciever antenna
WO2015200081A1 (en) * 2014-06-23 2015-12-30 Raytheon Company Magnetic antennas for ultra low frequency and very low frequency radiation

Cited By (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3066292A (en) * 1954-10-05 1962-11-27 Casco Products Corp Automoble antenna with toroid coil and magnetic core
US2975421A (en) * 1956-02-28 1961-03-14 George D Chichester Magnetic antenna
US2996717A (en) * 1959-02-06 1961-08-15 Hazeltine Research Inc Wave focusing antenna
US3353132A (en) * 1965-05-27 1967-11-14 Gen Electric Leakage flux suppressor windings for transformers
US3495264A (en) * 1966-12-09 1970-02-10 Continental Electronics Mfg Loop antenna comprising plural helical coils on closed magnetic core
FR2608845A1 (en) * 1986-12-22 1988-06-24 Pizon Ernest Receiving or transmitting antenna esp. for car radio - has prim. winding of coupling transformer inserted into loop formed by windings on rectangular ferrite bars
US5023585A (en) * 1988-11-17 1991-06-11 Murata Manufacturing Co., Ltd. Common-mode choking coil
US20030132889A1 (en) * 2002-01-04 2003-07-17 Darfon Electronics Copr. Loop antenna
US6822614B2 (en) * 2002-01-04 2004-11-23 Darfon Electronics Corp. Loop antenna
US20150207232A1 (en) * 2014-01-20 2015-07-23 Raytheon Company High efficiency polarized ulf/vlf/rf transciever antenna
WO2015109205A1 (en) * 2014-01-20 2015-07-23 Raytheon Company High efficiency polarized ulf/vlf/rf transciever antenna
US9831925B2 (en) * 2014-01-20 2017-11-28 Raytheon Company High efficiency polarized ULF/VLF/RF transciever antenna
WO2015200081A1 (en) * 2014-06-23 2015-12-30 Raytheon Company Magnetic antennas for ultra low frequency and very low frequency radiation
US9755765B2 (en) 2014-06-23 2017-09-05 Raytheon Company Magnetic antennas for ultra low frequency and very low frequency radiation

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