US2268782A - High frequency iron core - Google Patents
High frequency iron core Download PDFInfo
- Publication number
- US2268782A US2268782A US308813A US30881339A US2268782A US 2268782 A US2268782 A US 2268782A US 308813 A US308813 A US 308813A US 30881339 A US30881339 A US 30881339A US 2268782 A US2268782 A US 2268782A
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- US
- United States
- Prior art keywords
- high frequency
- core
- iron core
- frequency iron
- dielectric
- 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
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/20—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of particles, e.g. powder
- H01F1/22—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of particles, e.g. powder pressed, sintered, or bound together
- H01F1/24—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of particles, e.g. powder pressed, sintered, or bound together the particles being insulated
Definitions
- the dielectric constant of the mass core (pressed material or sprayed material) is very high and furthermore has often a very high temperature coefilcient, the dielectric behavior of the mass core is found to be an inconlic feature when the core is to serve for determining the frequency particularly in the case of short waves. It would as such be conceivable to shield the core against electric field lines by means of an electrically conducting sheet metal mantle but in this case an additional element of the structure is required, namely, the shielding mantle.
- an electrically semi-conducting binding means is employed in a high frequency iron core consisting of finely distributed iron powder and a binder. It is possible for instance to add carbon in an extremely fine distribution of the type used for making resistance layers.
- the conductivity becomes essentially greaterthan the wattless conduction value of the capacity which is formed by the iron core as the dielectric, yet not as high as conductivity of the iron, the dielectric behavior is no longer of importance. Hence, dielectric losses occur no longer.
- the upper limit for the value of the conduction lies in the additional damping which is caused in the core by the eddy currents due to the conduction. This limit is determined by the respectively prevailing frequency range and dielectric constant of the material and can be maintained within reasonable limits. Hence, the conductivity of the entire iron core is given a value such that the eddy losses are still permissible and the dielectric losses are diminished in view of the conducting shunt.
- a core for a high frequency inductance device composed of compressed finely divided magnetic material mixed with a semi-conducting binder, said binder being composed of insulation material mixed with finely divided carbon.
- a core for a high frequency inductance device composed of finely divided iron mixed with a binder which has finely divided carbo'n dispersed throughout it.
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- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Soft Magnetic Materials (AREA)
Description
Filed Dec. 12, 1939 iNVENTOR HERMANN ST/ER ATTORNEY Patented Jan. 6, 1942 HIGH FREQUENCY IRON CORE Hermann Stier, Berlin, Germany, asslgnor to -Telefnnken Gesellschaft fiir Drahtlose Telegraphic in. b. 11., Berlin, Germany, a corporation of Germany Application December 12, 1939, Serial No. 308,813 In Germany November 25, 1938 2 Claims.
when mass cores are used for high frequency coils the core aside from being permeated by magnetic lines of force is also permeated by electric lines of force. In the figure wherein the coil is designated by Sp and the core by K, such an electric field line is shown in dotted lines.
Since the dielectric constant of the mass core (pressed material or sprayed material) is very high and furthermore has often a very high temperature coefilcient, the dielectric behavior of the mass core is found to be an inconvient feature when the core is to serve for determining the frequency particularly in the case of short waves. It would as such be conceivable to shield the core against electric field lines by means of an electrically conducting sheet metal mantle but in this case an additional element of the structure is required, namely, the shielding mantle.
In accordance with the invention in a high frequency iron core consisting of finely distributed iron powder and a binder, an electrically semi-conducting binding means is employed. It is possible for instance to add carbon in an extremely fine distribution of the type used for making resistance layers.
It in using the invention the conductivity becomes essentially greaterthan the wattless conduction value of the capacity which is formed by the iron core as the dielectric, yet not as high as conductivity of the iron, the dielectric behavior is no longer of importance. Hence, dielectric losses occur no longer. The upper limit for the value of the conduction lies in the additional damping which is caused in the core by the eddy currents due to the conduction. This limit is determined by the respectively prevailing frequency range and dielectric constant of the material and can be maintained within reasonable limits. Hence, the conductivity of the entire iron core is given a value such that the eddy losses are still permissible and the dielectric losses are diminished in view of the conducting shunt.
Moreover, it will be sufilcient if only the exterior layer of the core is devised in the manner according to the invention. But in this case the making of the core meets with difiiculties.
I claim:
1. A core for a high frequency inductance device composed of compressed finely divided magnetic material mixed with a semi-conducting binder, said binder being composed of insulation material mixed with finely divided carbon.
2. A core for a high frequency inductance device composed of finely divided iron mixed with a binder which has finely divided carbo'n dispersed throughout it.
- HERMANN STIER.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE2268782X | 1938-11-25 |
Publications (1)
Publication Number | Publication Date |
---|---|
US2268782A true US2268782A (en) | 1942-01-06 |
Family
ID=7993120
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US308813A Expired - Lifetime US2268782A (en) | 1938-11-25 | 1939-12-12 | High frequency iron core |
Country Status (1)
Country | Link |
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US (1) | US2268782A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2597237A (en) * | 1948-06-25 | 1952-05-20 | Rca Corp | Variable loss paramagnetic cores |
US2597236A (en) * | 1947-10-24 | 1952-05-20 | Rca Corp | Comminuted ferromagnetic cores |
US3098761A (en) * | 1959-04-15 | 1963-07-23 | Westcott Horace Clifford | Magnetic recording element containing diamagnetic material |
-
1939
- 1939-12-12 US US308813A patent/US2268782A/en not_active Expired - Lifetime
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2597236A (en) * | 1947-10-24 | 1952-05-20 | Rca Corp | Comminuted ferromagnetic cores |
US2597237A (en) * | 1948-06-25 | 1952-05-20 | Rca Corp | Variable loss paramagnetic cores |
US3098761A (en) * | 1959-04-15 | 1963-07-23 | Westcott Horace Clifford | Magnetic recording element containing diamagnetic material |
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