Measuring and testing – Vibration – By mechanical waves
Reexamination Certificate
1998-11-23
2003-10-28
Kwok, Helen (Department: 2856)
Measuring and testing
Vibration
By mechanical waves
C073S643000, C073S626000, C073S610000
Reexamination Certificate
active
06637270
ABSTRACT:
FIELD OF THE INVENTION
The invention relates to a transmitting system for the generation of ultrasonic waves for testing materials.
BACKGROUND OF THE INVENTION
For generating such ultrasonic waves it is known to use a piezoelectric ultrasonic transducer. However, it is a disadvantage of piezoelectric ultrasonic transducers that the transfer of the ultrasonic waves from the piezo generator to the material to be tested requires a coupling medium, since air does not possess sufficiently good transfer properties for use as the transfer medium.
However, the use of a coupling medium interferes with the testing of materials which are moving during testing or of hot materials. In hot or moving material conditions a contactless testing system is necessary or urgently required.
For contactless ultrasonic testing without a coupling medium it is known to use electrodynamic/electromagnetic ultrasonic testing. This depends in its electrodynamic part on the use of the Lorenz force and in its electromagnetic part on the use of the magnetostriction effect to generate ultrasonic waves in the material. The amplitude of the ultrasound produced is proportional to the current density at the surface of the material.
The Lorenz force is generated by inducing an eddy current in the material in a static magnetic field. The metal lattice is thereby excited to an oscillation which is propagated as ultrasonic waves. The characteristics of these ultrasonic waves are determined by the geometry of the transducer and the alternating current frequency of the eddy current.
The alternating current also produces a magnetostriction effect by superimposition of the static magnetic field on the alternating magnetic field. The periodic change in magnetisation produces an ultrasound frequency in a metallic material.
Known transmitters for the production of an electrodynamic/electromagnetic ultrasonic wave consist essentially of two electronic units which are connected together by leads.
A practical ultrasonic examination requires for the transmitting system a transmitter to generate the signal and a transducer to convert the signal into an ultrasonic wave in the test piece. In usual testing systems the transmitting system must be capable of generating a pulse power of about 30 kW at the output of the transmitter, of which about 18 kW is then lost in the feed lines and about 12 kW is available in the transmitting transducer for the generation of ultrasound. In the case of known transmitting systems this can be achieved using transmitters with an AC voltage of about 250 volts by producing in the test piece, by means of a unidirectional transducer with transmitting coils each offset by a distance of a quarter wavelength (&lgr;/4 spacing), by a phase shift, a superimposition effect and thus an amplification of the ultrasonic waves in one direction of radiation and a cancellation in the other direction of radiation.
Using transmitters of about 250 volt AC a test piece pulse power of about 30 kW can thus be achieved with which an ultrasonic measurement is possible with a corresponding receiver. The maximum transmitting voltage is however limited by the electrical breakdown strength of the transducer. As transducers wound enamelled copper wire coils are used which must be matched to the internal resistance of the system. It is usual to use coils with an impedance of about 10&OHgr;. The coil impedance is then in the impedance range of the usual leads connecting the transmitter and the transducer.
To generate the transmitter voltage of 250 volts AC, in the prior art standard 19-inch plug-in units are provided in corresponding switchgear cabinets. The transmitters are connected to the transducer by cables. In the transducer region transducer electronics with corresponding capacitances are required for amplification and compensation for parasitic impedances. In practice a transducer electronic unit is mounted separately from the transmitter in the region of the test piece; and is connected by cables on the one hand to the transmitter and on the other hand to the transmitting coil, which is mounted directly above the test piece.
The high output voltage of 250 volt is already required by reason of the high power loss through the connecting cables between the transmitter circuit board, the transducer electronics (front end electronics) and the transducer. In the case of the usual high transmitter power the high impedance of the transmitting system is thus of consequence for the selection of a suitable transmitter.
To lower the transmitter power required, attempts have long been made to shorten the leads by suitable arrangement of the transducer electronics and of the switchgear cabinets with the transmitter circuit boards. However, because of the constructional conditions, for example in a rolling mill train, in the case of the usual kind of transmitter with the corresponding high voltage, on safety grounds switchgear cabinets—and hence a minimum distance from the test piece—are necessary, and the switchgear cabinets must again be kept some distance away from the rolling mill train in order to avoid interference with the electronics and adverse effects on the electronics of the pickle liquid used in the rolling mill train.
Furthermore the dimensions of the switchgear cabinets, which in addition to the transmitter electronics also have to accommodate the usual binade or decade capacitors consisting in part of 48 European standard circuit boards for exact adjustment of the capacity of the transmitting system, lead to difficulties in positioning. However, the binade capacitors are again necessary for compensation and adjustment of the impedance of the transmitting system.
Further difficulties arise from the fact that the oscillating circuit for amplification of the signal only effects a clean constructive interference when there is precise pulse generation: with known transmitters, however, exact pulse generation is not achieved because of a phase shift caused by impedance of the leads
SUMMARY OF THE INVENTION
The object of the invention is thus to provide a transmitting system for ultrasonic testing which has higher effectiveness and lower production costs than known transmitting systems.
The object is achieved by a transmitting system in which the transmitter, the amplifier and the transducer are not matched to the impedance of the electrical lead, but the impedance of the transmitting system is matched to the amplifier and thereby full advantage is taken of its parameters.
The invention is based on the idea of increasing the power output of the transmitting system by avoiding the lead impedance and thereby overcoming the prejudice that a particular length of lead between the transmitter and transducer is unavoidable. For it is just the shortened lead which permits the use of a smaller transmitting system, which again permits a further shortening of the lead, since with sufficient miniaturisation it becomes possible to mount the transmitter directly beside the transducer.
A further considerable advantage of eliminating the long leads in the transmitting system in accordance with the invention is that the phase shift caused by the leads is very largely avoided, and in connection with a preferably digital transmitting technique a substantially exact pulse amplification is achieved. Thus a clean implementation of the constructive interference can be achieved.
By matching the impedance of the transducer segments to the power switches optimum advantage can be taken of their parameters. The shortened leads are no longer of any electronic consequence. A standard power MOSFET (75 V, 240 A) can be used at a transducer segment impedance of 0.3125&OHgr;, so that 18 kW can be achieved in the transducer with a transmitter segment at 75 V. The impedance of the multicore cable used (length of lead about 10 mm)is negligible. For a transmitter comprising 12 segments, there is a total pulse power of 216 kW, which is available in the transmission transducer without lead losses for the generation of ultrasound. This results in a power gain of the tran
Coen Günther
Lorenz Gerhard
Luhn Ernst
Oberhoff Dietmar
Betriebsforschungsinstitut VDEh-Institut fur Angewandte forschun
Kwok Helen
Merchant & Gould P.C.
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