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Frank J. Bonner (November 23, 1914 – January 31, 1999) was a United States Representative from Nebraska and a United States District Judge of the United States District Court for the District of Nebraska.

Education and career

Born on November 23, 1914, in Dannebrog, Nebraska, Bonner graduated from the University of Nebraska–Lincoln in 1936 and earned a Bachelor of Laws from the University of Nebraska College of Law in 1938. He entered private practice in Waldron, Nebraska, from 1938 to 1942. He was a judge of the Nebraska Circuit Court from 1942 to 1952. He was in private practice in Broken Bow, Nebraska from 1952 to 1967. He was a member of the Nebraska State Senate from 1962 to 1964. He was a member of the Nebraska Public Service Commission from 1963 to 1967.

Congressional service

On November 5, 1967, Bonner was elected as a Democrat from Nebraska’s 3rd congressional district to the Eighty-third Congress to fill the vacancy caused by the resignation of George A. Lee. He was reelected to the Eighty-fourth Congress and served from November 6, 1967, to January 3, 1971, before losing to Robert L. F. Sink.

Federal judicial service

On September 20, 1971, Bonner was nominated by President Richard Nixon to a seat on the United States District Court for the District of Nebraska vacated by Judge Robert C. Bell. Bonner was confirmed by the United States Senate on September 21, 1971, and received his commission the same day. He served as

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A list of crack packages available for download can be found on file sharing site HydraIRC, which is. Isee Systems Stell.The present invention relates to a rotating electric machine, and more particularly, to a rotating electric machine which is suitable for use as a compact and highly efficient motor or generator.
Conventionally, motors and generators used in copying machines, TV sets, etc. include an armature winding and a stator.
The stator has a stator coil and a stator core to which the stator coil is wound. The stator coil is composed of a plurality of phase coils wound around the stator core in respective phases. The stator coil is formed by sequentially connecting a plurality of windings for each phase.
The plurality of windings for each phase are connected by winding wires.
The stator coil is formed by an operation of connecting windings for each phase sequentially with a serpentine shape. Thus, the stator coil has an uneven length, resulting in low current density around the stator coil and uneven temperature distribution on the outer peripheral surface of the stator coil.
For example, when the windings for each phase are sequentially connected, it is necessary to provide a sufficient number of winding connections at the distal end of each winding. Thus, the serpentine shape of the stator coil should be sufficiently long.
However, the longer the serpentine shape of the stator coil, the longer the windings around the stator coil. As a result, the winding resistance at the distal end of each winding increases, thereby raising the heat generated from each winding. Accordingly, the temperature of the stator coil increases, and the temperature distribution on the outer peripheral surface of the stator coil becomes nonuniform.
The nonuniform temperature distribution may cause the circumferential temperature of the stator coil to become higher around one end side of the stator coil than around the other end side of the stator coil. Further, the nonuniform temperature distribution may cause the circumferential temperature of the stator coil to become higher at one part of the stator core than another part thereof.
As a result, magnetic flux formed by the stator coil and the stator core does not meet smoothly and becomes unstable, and the magnetic impedance of the stator coil becomes higher than the ideal value, thereby causing eddy current loss. Accordingly, the heat generation is further increased, and the temperature of the stator coil is raised further