US3491320A - Tuning coil with movable magnetic core - Google Patents

Tuning coil with movable magnetic core Download PDF

Info

Publication number
US3491320A
US3491320A US798254*A US3491320DA US3491320A US 3491320 A US3491320 A US 3491320A US 3491320D A US3491320D A US 3491320DA US 3491320 A US3491320 A US 3491320A
Authority
US
United States
Prior art keywords
core
coil
tuning
sleeve
magnetic core
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
US798254*A
Inventor
Tamaki Ohashi
Takeshi Ishino
Isao Yokoyama
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
TDK Corp
Original Assignee
TDK Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by TDK Corp filed Critical TDK Corp
Application granted granted Critical
Publication of US3491320A publication Critical patent/US3491320A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F21/00Variable inductances or transformers of the signal type
    • H01F21/02Variable inductances or transformers of the signal type continuously variable, e.g. variometers
    • H01F21/06Variable inductances or transformers of the signal type continuously variable, e.g. variometers by movement of core or part of core relative to the windings as a whole

Definitions

  • variable inductance coil including a solenoid type coil, an adjusting core made of magnetic material and mounted for axial movement relative to the coil, and a fixed magnetic sleeve disposed around the coil to enclose the same.
  • the fixed magnetic sleeve extends longitudinally beyond the coil at the end where the adjusting core is located so that the fluctuation of the electric characteristics of the adjusting core is minimized.
  • This invention relates to a variable inductance (,u tuning) coil to be used in a method of a tuning system, for example, in a car radio set.
  • a dust core has been used exclusively for a conventional variable inductance coil.
  • the temperature coefiicient is small, and that applicable frequency band is wide.
  • its permeability is so low that the long stroke, as the variable inductance, is essential to cover a certain tuning frequency range, the gap between the sleeve core and adjusting core must be small and the close tolerance of the cores must be required.
  • a coil 2 is wound on a bobbin 1
  • a fixed magnetic sleeve core 3 (which shall be known as a sleeve core hereinafter) shorter than the coil 2 is applied outside the said coil and a shield case 4 is further applied outside the said sleeve core so that an adjusting core (moving core) 5 for tuning may be moved in the directions indicated by the arrows x and x for tuning.
  • the tuner for the car radio set has an antenna coil, tuning coil and oscillating coil or further a high frequency amplifying c-oil.
  • the permeability of the adjusting core is fluctuated, the position of the adjusting core is also fluctuated in case of obtaining the same inductance. Consequently, in mass-produced sets incorporating such a kind of cores, the frequency f-stroke L curves as shown, for example, in FIG. 2 of these tuners do not agree with each other.
  • the curve of each coil in one tuner does not become parallel. Therefore, there is a great defect that, in case they are incorporated into radios, tracking will become diflicult. For example, in case, in FIG.
  • the core 5 is of a diameter of '5 mm. and a length of 30 mm. and the sleeve core 3 is of an outside diameter of 15 mm., an inside diameter of 12 mm. and a length of 14 mm, the average tuning frequency by the stroke L of the tuning core 5 and five tuning cores will be :as shown in FIG. 2.
  • FIG. 3 shows the fluctuation of the tuning frequency by a range R.
  • the curve 10 represents the fluctuation of the tuning frequency of the same as is shown in FIG. 2 and the curve 11 represents the case according to the present invention.
  • the fluctuation between respective samples will be of a considerably large value as shown by the curve 10.
  • tracking has been diflicult.
  • notches 6 and 6' have been made in a part of the adjusting core 5 or, as shown in FIG- 5, the winding pitch of the coil 2 has been varied.
  • the operation has been complicated, the production cost has been high and yet no sufficient effect has been obtained.
  • the interaction between the sleeve core and the adjusting core have been investigated on the permeability of the cores and the relative positioning.
  • the sleeve core 3 is made longer by k than the coil 2 and
  • FIG. 7 shows the fluctuationR-stroke L as parameter k, which is shown in FIG. 6.
  • the fluctuation of the inductance of the variable inductance coil can be made small and tracking can be made easy.
  • a variable inductance coil comprising a single solenoid type coil wound on a fixed hollow bobbin, said single coil being wound with uniform spacing over its entire length, an adjustable core made of magnetic material and mounted for axial movement within one end of said hollow bobbin relative to said coil, a. fixed magnetic sleeve disposed around said coil and made of ferrite having a permeability of more than 50 and greater than the permeability of said core, said sleeve extending beyond said coil by a distance sufficientto minimize fluctuations in the tuning frequency of said coil, and a shield casing disposed around said fixed magnetic sleeve.

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Coils Or Transformers For Communication (AREA)

Description

Jan. 20,1970 TAMAKI oH sm EITAL 3,491,320
TUNING COIL WITH MOVABLE MAGNETIC CORE Criginal Filed March 29, 1967 3 Sheets-Sheet l F/g. PR/OR ART 2 PR/OR ART l6 f (X'lOOK /s) |4 1'0 2'0 5 0 L (mm) INVENTORS TAMAKI OHASHI TAKESHI ISHlNO IsAo YOKOYAMA ATTY6.
Jan. 20,1976 TAMAKI OHASHI ETAL 3,491,320
TUNING COIL WITH MOVABLE MAGNETIC CORE Original Filed March 29, 1967 3 Sheets-Sheet 2 R 3 PR/OR ART 6 v 4- IO (0 2'0 30 L (mm) 4 5 PRIOR ART PRIOR ART 2 Mill/fir INVENTORS TAMAKI OHASH TAKESHI ISl-HNO IsAo YOKOVAMA 5J3 W0%) W7 ATTYS,
Jam. 20,1970 TAMAKI oHAsm L 3,491,320
TUNING con; wxwa MOVABLE mimic CORE Original Filed March 29, 1967 a Sheets-Sheet s INVENTORS TAMAK/ OHASHI TAKESHI ISHINO I SAO YOKOYAMA Arrvs.
United States Patent TUNING COIL WITH MOVABLE MAGNETIC CORE Tamaki Ohashi, Tokyo, and Takeshi lshino and Isao Yokoyama, Akita-ken, Japan, assignors to TDK Electronics Co., Ltd., Tokyo, Japan, a corporation of Japan Continuation of application Ser. No. 626,742, Mar. 29,
1967. This application Jan. 31, 1969, Ser. No. 798,254 Int. Cl. H01f 21/10, 21/06 US. Cl. 336-87 1 Claim ABSTRACT OF THE DISCLOSURE A variable inductance coil including a solenoid type coil, an adjusting core made of magnetic material and mounted for axial movement relative to the coil, and a fixed magnetic sleeve disposed around the coil to enclose the same. The fixed magnetic sleeve extends longitudinally beyond the coil at the end where the adjusting core is located so that the fluctuation of the electric characteristics of the adjusting core is minimized.
This application is a continuation of application Ser. No. 626,742, filed Mar. 29, 1967, now abandoned.
This invention relates to a variable inductance (,u tuning) coil to be used in a method of a tuning system, for example, in a car radio set.
A dust core has been used exclusively for a conventional variable inductance coil. As the advantages of such a dust core, it can be enumerated that the temperature coefiicient is small, and that applicable frequency band is wide. On the other hand, its permeability is so low that the long stroke, as the variable inductance, is essential to cover a certain tuning frequency range, the gap between the sleeve core and adjusting core must be small and the close tolerance of the cores must be required.
Instead of the above described dust cores, there have been used ferrite core in Japan since some time ago to eliminate the defects of such dust cores. However, inherently ferrite is a material so high in the permeability that there have been many faults due to unknown factors and have been much troublesome especially in the tracking process of the radio set production.
As illustrated in FIG. 1, in a conventional ferrite variable inductance coil, a coil 2 is wound on a bobbin 1, a fixed magnetic sleeve core 3 (which shall be known as a sleeve core hereinafter) shorter than the coil 2 is applied outside the said coil and a shield case 4 is further applied outside the said sleeve core so that an adjusting core (moving core) 5 for tuning may be moved in the directions indicated by the arrows x and x for tuning.
Usually, the tuner for the car radio set has an antenna coil, tuning coil and oscillating coil or further a high frequency amplifying c-oil. As in adjusting them the permeability of the adjusting core is fluctuated, the position of the adjusting core is also fluctuated in case of obtaining the same inductance. Consequently, in mass-produced sets incorporating such a kind of cores, the frequency f-stroke L curves as shown, for example, in FIG. 2 of these tuners do not agree with each other. Besides, the curve of each coil in one tuner does not become parallel. Therefore, there is a great defect that, in case they are incorporated into radios, tracking will become diflicult. For example, in case, in FIG. 1, the core 5 is of a diameter of '5 mm. and a length of 30 mm. and the sleeve core 3 is of an outside diameter of 15 mm., an inside diameter of 12 mm. and a length of 14 mm, the average tuning frequency by the stroke L of the tuning core 5 and five tuning cores will be :as shown in FIG. 2. FIG. 3 shows the fluctuation of the tuning frequency by a range R. In FIG. 3, the curve 10 represents the fluctuation of the tuning frequency of the same as is shown in FIG. 2 and the curve 11 represents the case according to the present invention. As evident from FIG. 2 and the curve 10 in FIG. 3, even if the dimension allowance is $0.05 mm., the fluctuation between respective samples will be of a considerably large value as shown by the curve 10. Thus tracking has been diflicult.
As a countermeasure against it, as shown in FIG. 4, notches 6 and 6' have been made in a part of the adjusting core 5 or, as shown in FIG- 5, the winding pitch of the coil 2 has been varied. However, in either manner, the operation has been complicated, the production cost has been high and yet no sufficient effect has been obtained.
In the present invention, in order to reduce such fluctuation, the interaction between the sleeve core and the adjusting core have been investigated on the permeability of the cores and the relative positioning. In the present invention, as shown in FIG. 6, the sleeve core 3 is made longer by k than the coil 2 and FIG. 7 shows the fluctuationR-stroke L as parameter k, which is shown in FIG. 6.
In FIG. 7, the curves A, B and C represent fluctuations in case dust cores having a value of ,u =20 were used for the sleeve core and adjusting core. It is found that, when the value of k of the sleeve core was varied to 0 mm. (represented by the curve A), 5 mm. (represented by the curve B) and 10 mm. (represented by the curve C), the reduction of the fluctuation was shown as the value of k was varied toward k: 10 mm., and the deviation was 4 kc./ sec. in the value of k=10 mm. On the other hand, when only the sleeve core was made from the material of :450, the fluctuation reduced gradually as in 0, 2, 4, 6, 8 and 10 mm. in FIG. 7, and was of a practically satisfactory value at k: 10 mm.
From the above, if ,u, of the material of the sleeve core is made as large as possible, m of the adjusting core is made small and the length of the sleeve core is made longer than the coil, the fluctuation of tuning frequency will be minimized. Therefore, in the variable inductance coil represented by the curve 10 in FIG. 3, in case the adjusting core was made from dust core and the sleeve core (of :50) was made from ferrite 3 mm. longer than the coil, the fluctuation R was as in the curve 11 in FIG. 3.
As described above, according to the present invention, by means of making the permeability ,u, of the material of the sleeve core more than 50 and making the sleeve core slightly longer than the coil, the fluctuation of the inductance of the variable inductance coil can be made small and tracking can be made easy.
While there has been described in connection with the preferred embodiment of this invention, it will be obvious to those skilled in the art that various changes and modifications may be made therein without departing from the invention, and it is aimed, therefore, to cover in the appended claim all such changes and modifications as fall within the true spirit and scope of the invention.
We claim as our invention.
1. A variable inductance coil comprising a single solenoid type coil wound on a fixed hollow bobbin, said single coil being wound with uniform spacing over its entire length, an adjustable core made of magnetic material and mounted for axial movement within one end of said hollow bobbin relative to said coil, a. fixed magnetic sleeve disposed around said coil and made of ferrite having a permeability of more than 50 and greater than the permeability of said core, said sleeve extending beyond said coil by a distance sufficientto minimize fluctuations in the tuning frequency of said coil, and a shield casing disposed around said fixed magnetic sleeve.
References Cited UNITED STATES PATENTS Weis 336134 Harvey 33687 Berg 336132 XR OTHER REFERENCES Bozorth: Ferromagnetism, D. Van Nostrand Company Inc., March 1951, pp. 246 and 870-871.
THOMAS J. KOZMA, Primary Examiner US. Cl. X.R.
Conradet a1 336136XR 10 336432 136
US798254*A 1969-01-31 1969-01-31 Tuning coil with movable magnetic core Expired - Lifetime US3491320A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US79825469A 1969-01-31 1969-01-31

Publications (1)

Publication Number Publication Date
US3491320A true US3491320A (en) 1970-01-20

Family

ID=25172917

Family Applications (1)

Application Number Title Priority Date Filing Date
US798254*A Expired - Lifetime US3491320A (en) 1969-01-31 1969-01-31 Tuning coil with movable magnetic core

Country Status (1)

Country Link
US (1) US3491320A (en)

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2144353A (en) * 1935-01-08 1939-01-17 Siemens Ag Variable inductance device
US2283924A (en) * 1935-12-31 1942-05-26 Rca Corp Magnetically tuned high frequency circuits
US2407916A (en) * 1943-04-10 1946-09-17 Stewart Warner Corp Shielded coil
US2430757A (en) * 1944-11-14 1947-11-11 Manning Maxwell & Moore Inc Electrical remote-reading positionindicating apparatus
US2597237A (en) * 1948-06-25 1952-05-20 Rca Corp Variable loss paramagnetic cores
US2630560A (en) * 1949-04-05 1953-03-03 Sylvania Electric Prod Radio-frequency transformer

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2144353A (en) * 1935-01-08 1939-01-17 Siemens Ag Variable inductance device
US2283924A (en) * 1935-12-31 1942-05-26 Rca Corp Magnetically tuned high frequency circuits
US2407916A (en) * 1943-04-10 1946-09-17 Stewart Warner Corp Shielded coil
US2430757A (en) * 1944-11-14 1947-11-11 Manning Maxwell & Moore Inc Electrical remote-reading positionindicating apparatus
US2597237A (en) * 1948-06-25 1952-05-20 Rca Corp Variable loss paramagnetic cores
US2630560A (en) * 1949-04-05 1953-03-03 Sylvania Electric Prod Radio-frequency transformer

Similar Documents

Publication Publication Date Title
US4459570A (en) Ultra-high frequency filter with a dielectric resonator tunable in a large band width
US2180413A (en) Magnetically tuned high frequency circuits
US2375309A (en) High-frequency transformer
US3358256A (en) Miniature low frequency transformer
US2748386A (en) Antenna systems
US2370714A (en) Variable permeability tuning device
US2748357A (en) Tunable inductor
US3238484A (en) D-cores with associated windings for producing high q
US2051012A (en) Permeability tuning means
US2283924A (en) Magnetically tuned high frequency circuits
US2340749A (en) Variable permeability tuning system
US3491320A (en) Tuning coil with movable magnetic core
US2354365A (en) Coupling device for adjustable coupling systems
US2567394A (en) Inductance coil
US2882392A (en) Receiver tuned by inductors with tracking by initial positionment of coils on cores
US2489114A (en) Variable inductance device
US2568310A (en) Inductance coil structure
US2141573A (en) Antenna coupling system
US2234002A (en) Temperature compensated magnetic core inductor
US2483900A (en) Coil having a ferrite core
US2059393A (en) Magnetic core for high frequency inductances
US2064772A (en) High-frequency coil with adjustable inductance value
US2598810A (en) Wide range high-frequency tuner
US2730681A (en) Inductance
US2714187A (en) Variable high frequency coupling transformer