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The London moment (after ) is a quantum-mechanical whereby a generates a whose axis lines up exactly with the spin axis."Towards a new test of general relativity." Physorg Retrieved 10 March 2011 The term may also refer to the of any of any , caused by the lagging behind the rotation of the object, although the field strength is independent of the charge carrier density in the superconductor.


Gravity Probe B
A determines the orientation of the generated field, which is to determine the axis of rotation. Gyroscopes of this type can be extremely accurate and stable. For example, those used in the Gravity Probe B experiment measured changes in gyroscope spin axis orientation to better than 0.5 milliarcseconds (1.4 degrees) over a one-year period. Einstein.stanford.edu This is equivalent to an angular separation the width of a human hair viewed from 32 kilometers (20 miles) away.

The GP-B gyro consists of a near-perfect spherical rotating mass made of , which provides a support for a thin layer of material. To eliminate friction found in conventional bearings, the rotor assembly is centered by the electric field from six electrodes. After the initial spin-up by a jet of helium which brings the rotor to 4,000 RPM, the polished gyroscope housing is evacuated to an ultra-high vacuum to further reduce drag on the rotor. Provided the suspension electronics remain powered, the extreme rotational symmetry, lack of friction, and low drag will allow the angular momentum of the rotor to keep it spinning for about 15,000 years. Einstein.stanford.edu

A sensitive DC magnetometer able to discriminate changes as small as one quantum, or about , is used to monitor the gyroscope. A precession, or tilt, in the orientation of the rotor causes the London moment to shift relative to the housing. The moving field passes through a superconducting fixed to the housing, inducing a small electric current. The current produces a voltage across a shunt resistance, which is resolved to spherical coordinates by a microprocessor. The system is designed to minimize on the rotor. Einstein.stanford.edu


Magnetic field strength
The magnetic field strength associated with a rotating superconductor is given by:
B=-\frac{2M }{Q}\ \omega ,
where M and Q are the mass and the charge of the superconducting charge carriers respectively. For the case of of electrons, and . Despite the electrons existing in a strongly interacting environment, me denotes here the mass of the bare electrons (as in vacuum), and not e.g. the effective mass of conducting electrons of the normal phase.


Etymology
Named for the physical scientist , and moment as in .


See also

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