Bbc Brown, Boveri & Company, Limited

Pierre Keller

Gerold Brandli

Werner Buser

Walter Munch

A method and apparatus for monitoring the state of the surface of a moving body wherein a four-terminal eddy-current coil circuit is connected in a feedback loop of an RC resonator. The eddy-current coil circuit is placed in proximity to the monitored surface of the moving body and connected in the feedback loop of an RC resonator such that a change in the state of the surface of the moving body results in a change in the conductivity thereof, which conductivity change produces a phase displacement changing the output frequency of the RC resonator. During operation, a first data set is obtained from the coil circuit and RC resonator presenting a first runout profile of the body when the monitored state is in an initial state. The first data set is stored in a memory, and a subsequent profile is derived to obtain a second data set indicative of the operational state of the surface of the moving body. The second data set is also stored in the memory and then the first data set is subtracted from the second data set to obtain an effective or true profile of the surface of the body at the subsequent operational time.

Determining the state of the surface of a moving body using eddy

A method for contactless measurement of conductivity and/or temperature on metals by means of the eddy current effect induced within the metal by an alternating magnetic field produced by an excitation coil fed with alternating current arranged with its axis perpendicular to the surface of the metallic test specimen, there being in addition to the excitation coil a pair of measuring coils of equal radius arranged coaxially and symmetrically with respect to the excitation coil at each end respectively of the excitation coil and having an axial length substantially less than that of the excitation coil. The two measuring coils are connected electrically in series opposition and the phase angle between the current in the measuring coils and the current in the excitation coil is taken as an indication of the measured variable. In order to reduce the so-called 'lift-off' effect to a minimum and allow accurate contactless measurement such that substantial tolerances are permissible for the distance between the test specimen and measuring head which carries the coils, the radius between the excitation coil on the one hand, and the measuring coils on the other, is smaller than 1/4 or greater than 4, depending on whether the measuring coils are located respectively outside or inside the excitation coil, and the measuring head is at such a distance from the specimen surface that the phase angle between the excitation-coil signal and the measuring-coil signal exhibits a maximum.

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Baden, Switzerland

Pierre Keller