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Magnetic multi-turn absolute position detection device

ActiveUS20130169270A1Low magnetic disturbanceCancel magnetic interferenceElectric/magnetic position measurementsWork measurementPhysicsMagnet
The disclosure relates to a magnetic device for detecting the absolute position of an input shaft capable of rotating more than 360°, the device including a main magnetic sensor, a motion reducer, and a secondary magnetic sensor, wherein the main magnetic sensor is connected to a rotor, measures the rotation of the shaft for ranges of angles of less than 360°, and includes a main magnet, the motion reducer converts the rotation of the shaft into a reduced rotation, the maximum amplitude of which is equal to no more than 360°, and the secondary magnetic sensor measures the reduced rotation and includes a secondary magnet. According to the disclosure, the secondary magnet is arranged between the upper and lower planes of the main rotor, and the main magnet has P pairs of poles, where P is greater than 1.
Owner:MOVING MAGNET TECH

Microwave sealing for radar level gauges

A radar level gauge system is disclosed, having a transmitter for transmitting measuring signals towards the surface of the filling material, a receiver for receiving echo signals from said surface and a fastening structure adapted to secure said transmitter and receiver in a measuring position on a feed-through structure located in an upper boundary of said container. Further, a sealing unit is arranged between said fastening structure and said feed-through, and adapted to provide a pressure seal between the inside and the outside of the container, and in addition, there is provided means for blocking electromagnetic energy, adapted to block net transfer of electromagnetic energy between the inside and the outside of the container through said sealing unit.
Owner:ROSEMOUNT TANK RADAR

Externally Guided and Directed Field Induction Resistivity Tool

In one aspect an induction resistivity tool incorporated into a downhole tool string comprises an outer wall of a downhole component comprising an outer diameter and at least one induction transmitter assembly disposed along the outer diameter. The at least one transmitter assembly comprises at least one induction transmitter coil wound about at least one core. The at least one transmitter coil is adapted to project an induction signal outward from the outer wall when the at least one transmitter coil is carrying an electrical current. The transmitter assembly is adapted to create electromagnetic fields that originate the induction signal from outside the outer wall and substantially prevent the signal from entering the outer wall.
Owner:SCHLUMBERGER TECH CORP

Superconducting NMR resonators with macroscopically homogeneous superconductor distribution

An NMR resonator for receiving RF signals at desired resonance frequencies from a measuring sample in a volume under investigation disposed about a coordinate origin (x,y,z=0), with a means for producing a homogeneous magnetic field B.sub.0 in the direction of a z axis, wherein superconducting conductor structures are disposed between z=-.vertline.z.sub.1.vertline. and z=+.vertline.z.sub.2.vertline. on a surface which is translation-invariant (=z-invariant) in the z direction at a radial separation from the measuring sample, is characterized in that a compensation arrangement is additionally provided on the z-invariant surface, which extends to values of at least +.vertline.z.sub.2.vertline.+0.5.vertline.r.vertline.>z> -.vertline.z.sub.1.vertline.-0.5.vertline.r.vertline., wherein .vertline.r.vertline. is the minimum separation between the measuring sample and the compensation arrangement, wherein the compensation arrangement comprises further superconducting conductor structures which are RF-decoupled from the RF resonator, with the conductor structures of the compensation arrangement and of the RF resonator being composed of individual surface sections ("Z-structures") which comprise superconducting structures and are disposed in the z-invariant surface to each extend along the entire length in the z direction of the conductor structures of the compensation arrangement and of the RF resonator, those superconducting structures being disposed such that decomposition of the surface of the Z structures into a plurality of small equally sized surface elements and application of a homogeneous test magnetic field along the surface normal of each surface element for all surface elements which differ only with respect to their z position, induces a magnetic dipole moment of the same strength. In this manner, the disturbing influence caused by magnetization of the superconductor is very well compensated for.
Owner:BRUKER SWITZERLAND AG
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