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Publication numberUS2548598 A
Publication typeGrant
Publication dateApr 10, 1951
Filing dateFeb 17, 1950
Priority dateFeb 17, 1950
Publication numberUS 2548598 A, US 2548598A, US-A-2548598, US2548598 A, US2548598A
InventorsFeiker Jr George E
Original AssigneeGen Electric
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Apparatus for detection of flaws by means of microwaves
US 2548598 A
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Description  (OCR text may contain errors)

April 10., 1951 s E FEIKER JR APPARATUS. Fo'R DETEcTI'oN 0F FLAWS BY MEANS OF MICROWAVES Filed Feb. 17, 1950 OUTPUT HIGH FREQUENCY SIGNAL INPUT 0F WAVELENGTH? CRYSTAL DE TECTOR MOT/ ON OF WIRE Inventor: George E.FG'IKQY,JYT,

His Attorney Patented Apr. 10, 1 951 APPARATUS FOR DETECTION OF FLAWS BY MEANS OF MICROWAVES George E. Feiker, Jr., Albany, N. Y., assignor to General Electric Company, a corporation of New York Application February 17, 1950, Serial No. 144,630

3 Claims. (01. 175183) The presentinvention relates in general to apparatus for the, detection of flaws in conductors by means of electromagnetic waves and in particular relates to improvements in apparatus for the detection of flaws in wire-like conductors by means'of microwaves.

The invention may be used to detect occluded scale and surface imperfections, such as cuts and nicks, in aluminum wire, for instance.

Accordingly, it is a general object of my invention to provide means for the detection of flaws in conductors by means of electromagnetic waves.

It is a further object of my invention to provide a microwave flaw detector for the detection of flaws in conductors such as wire and the like.

The features of the invention desired to be protected are pointed out in the appended claims. The invention itself together with its further End portion 2 comprises/two members 5 and 6 together forming an end wall 2 with an opening for the insertion of a wire-like conductor l within the hollow member I and at the same time providing a high frequency choke means I by means of which high frequency energy is objects and advantages may best be understood by reference to the following description and to the single figure of the drawing which represents a cross-sectional view of the apparatus for carrying out my invention.

The invention is carried out in the embodiment shown in the drawing by means of a cavity resonator of which the wire-like conductor under test forms a part. The wire-like conductor is inserted into the cavity resonator through wall members which, form high frequency chokes with the wire-like conductor. The high frequency choke arrangement permits insertion of the conductor while at the same time prevents the escape of high frequency energy from the resonator. Means are provided for coupling signals into the resonator and for detecting and indicating the signal level in the resonator. As the .wire-like conductor isinserted or drawn through the resonator, an imperfection, such as occluded matter or cuts, causes a drop inthe signal level inthe resonator due to increased" resistive losses .introduced into the resonator or due to the detuning of the resonator caused by the cuts. Since the inner and outer conductors of the choke forming members are much closer together than in a normal resonator or transmission line, slight changes in cross section in the wire-like conductor which comprises part of the inner conductor of thechoke cause a considerable detuning of the choke and consequently of the cavity with a corresponding drop'in' signal level of the resonator.

Referring now with particularity to the single figure of the drawing, there is shown a generally cylindrical conductive hollow member I closed in with conductive end portions 2 and 3 to form a cavity resonator 4. Copper or brass or any similar material of good conductivity may be used in the construction of the resonator.

prevented from escaping from the cavity resonator 4. The inner memberi of end wall 2 comprises a cylindrically shaped conductor having a flanged portion 8 located at one end. The inner surface 9 of thecylindrical member 5 forms part of the outer conductor of the choke; the wire-like conductor 1- forms part of the inner conductor of the choke. The outer member 6 of the 'endwall 2 fits over the corresponding inner member 5 to form the re-entrant portion of the above referred to choke. The outer memher 6 comprises 53. hollow cylindrical'portion at one end of which is located a flange ID by means of which attachment is made to the flange portion 8- of the inner member 5. At the other end of the outer member is located an end wall H with a hole 12 adapted to pass the wire-like conductor 1. The inner and outer members 5 and. 6 are suitably fastened together and. to

the cylindrical member I at their respective flanged portions 8 and In as shown by soldering or clamping or by both soldering and clamping to form the end wall 2 of resonator 4. The end wall 3 member'is identical to end wall member 2. The hollow member I with the end walls 2 and 3 and the wire-like conductor 1 forms a cavity resonator 4 of the concentric line type. It should be noted that the characteristic impedance of the section of transmission line formed by the inner surface of 5 and the wirelike conductor is considerably smaller than the characteristic impedance of the section of transmission line forming the cavity resonator section proper since ratio of the inductance per unit length'to the capacity per unit length of transmission line is smaller. Because of the closeness of the inner and outer conductors in the choke portion .of the apparatus, a small nick or cut in the wire-like conductor 1 will produce a large percentage change in the spacing between inner and outer sections at that point to cause an appreciable discontinuity in the section of transmission line forming the choke and consequently detuning it. The detuning will be reflected in the resonator section and will be indicated as a change in the output level of the signal.

Means are provided for coupling a high frequency signal into the cavity resonator 4 and in the embodiment shown takes the form of a concentric transmission line I3 connected to a source of high frequency signal, the other end of which is connected to the cavity resonator 4 and is terminated in a loop l4. It will be apparent to by means of a similar loop which is connected: I

to a transmission line [6. It is apparent that other means of coupling energy from the reso nator may readily be utilized. The signal is detected by means of a rectifier i7 which'may be acrystal detector and appropriate detection circuits 3. In the embodiment shown, the one end 'of the crystal detector I! i s,, connected to the center conductor of the transmission line 16 and the other end is connected to the outer conductor of the transmission line [6 through a by-pass capacitor is, The signal level within the cavity resonator 4 is measured by microammeter 20. It is apparent to those skilled in the. art that other means may be used to detect changes. in the signal level within the cavity.

The apparatus. may be used for the detection of nonresistive as well as resistive flaws. Resistive flaws take the form of occluded scale in the wire. Nonresistive flaws. take. the form of nicks orcuts in the. wire. The apparatus may be operated at any suitable frequency at which the effectsto. be hereinafter described take place. It has been found that. 3,000 megacycles is quite satisfactory for practical purposes. It should be observed that the resonator 4 is one-half a wavelength long. at the, frequency of, operation of the apparatus. The resonator 4 is suitably excited by a microwave signal. With a section of wire 1 free. from defectsv in place as shown in the figure, the frequencyof the high frequency input signal is adjusted to give maximum rectified output at microammeter 28. If the wire i is moved axially through the cavity, a defect in the sur-. face willcause a drop in the detector output as it passes through the re-entrant choke. For slow passage of wire, this drop in output can be used as a visual indication of the flaw. For rapid passageof the wire, thechange in output can be used to trigger a relay after being suitably amplified. In order to facilitate amplification, the high frequency input can be amplitude modulated at an audio rate.

The principle of operation is as follows: At resonance, a large current flows radially in the end plates 8 of the cavity resonator 4. .This current must flow into the outer conductor of the re-entrant choke at point 21 and return by way of the wire "I. This large current is thus forced to flow across the surface imperfection. Two effects are possible. If the surface imperfection consists of occluded scale or other foreign substance, of a higher resistivity than the wire, the surface resistivity will be increased. Since the depth of current flow is very slight because of the use of high frequency excitation, this will cause an appreciable change in the losses in the re-entrant choke, which are a maximum at the high current point near 2|. With proper design, the change in losses is a large enough proportion of the total losses so that the change shows up as a transmission loss between input andoutput couplings l3 and I6, respectively. If, on the other hand, the surface imperfection is a nick in the otherwise smooth and pure material of the wire, the discontinuity in the char acteristic impedance as the wire passes through the choke will detune the cavity resonator 4, also resulting in a. change in detector output. Both effects may be present for a given imperfe'ction.

- The l e-entrant chokes are. made approxh mately one-quarter wavelength long as shown in the figure so that at point 22 the current flowing across the joint between wire and choke is a minimum. In this Way, changes in contact resistance due to passage of the wire through 'the guide hole 12 have no eifect on the output.

While I have shown and described a particular embodiment of my invention, it will be obvious to those skilled in the art that various changes and modifications may be made without departing from my invention and its broad aspects. I therefore aim in the appended claims to cover all such changes and modifications as fallwithin the true. spirit. a d scop o my in ntion,

Whatl claim, as. new and desire to secure by Letters Patent of the United States is:

,1. Detector apparatus for detecting flaws in wire-like conductors comprising a cavity resonator having walls of high current flow, choke means located in. two of said walls permitting the passage of said wire-like conductor through said cavity resonator, said choke means comprising with said wire-like conductor a section of short circuited transmission lines having a high current flow region adjacent said walls, means supplying high frequency signals to said cavity resonator, detecting means for detecting changes in the signal level due to imperfections in said wire-like conductor.

2. Detection apparatus, for the detection of flaws in wire-like. conductors by means of electromagnetic waves comprising a cylindrically shaped cavity resonator having an axial length of a multiple of a half wavelength at the frequency of said waves, choke means in. the end walls of said resonator permitting the passage of said wire-like conductor through said cavity, said choke means comprising with said wire-like conductor a section of short circuited transmission line having a high current flow region adjacent said wall, means supplying high frequency signals to said cavity resonator, detecting means for detecting changes in the signal level due to changes in the surfaces of said wire-like conductor.

3. Detection apparatus for the detection of flaws in wire-like conductors by means of high frequency currents comprising a hollow conductive member having end walls of high current flow, opening means in each of said end walls for the insertion of said wire-like conductors in said hollow member, said hollow member with said wire-like conductors forming a concentricline cavity resonator, said opening REFERENCES CITED The following references are of record in the file of this patent:

UNITED STATES PATENTS Number Name Date 2,456,012 Muskat et al. Dec. 14, 1948 2,491,418 Schlesman Dec. 13, 1949 2,503,256 Ginzton et al Apr. 11, 1950

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US2456012 *Dec 21, 1944Dec 14, 1948Gulf Research Development CoMethod of and apparatus for measuring the electrical properties and surface characteristics of materials
US2491418 *Apr 4, 1946Dec 13, 1949Socony Vacuum Oil Co IncAutomatic inspection device
US2503256 *Jan 29, 1943Apr 11, 1950Sperry CorpUltra high frequency wavemeter
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US2758188 *Aug 27, 1953Aug 7, 1956Westinghouse Electric CorpLevitation and heating of electrically conductive materials by means of electromagnetic resonators
US2788497 *May 31, 1951Apr 9, 1957Westinghouse Electric CorpRidged waveguide matching device
US3045146 *Mar 18, 1959Jul 17, 1962Eitel Mccullough IncTunable resonant cavity
US3082375 *Jul 5, 1960Mar 19, 1963Robert Mednick ITunable high frequency responsive device with shielded converter
US3384814 *Sep 25, 1963May 21, 1968Bell Telephone Labor IncRidge waveguide resonant cavity for measuring dielectric constants
US3458808 *May 26, 1965Jul 29, 1969Nils Bertil AgdurApparatus for measuring the properties of a material by resonance techniques
US3460031 *Jun 8, 1966Aug 5, 1969Industrial Nucleonics CorpMicrowave waveguide moisture measurement
US3525934 *May 24, 1967Aug 25, 1970Magnaflux CorpNondestructive microwave testing system for wire
US3541434 *Aug 25, 1966Nov 17, 1970Mc Donnell Douglas CorpApparatus for the broadband microwave determination of certain characteristics of substances
US3688188 *Dec 21, 1970Aug 29, 1972Bendix CorpMeans for measuring the density of fluid in a conduit
US3739263 *Sep 27, 1971Jun 12, 1973Inst MikrovagsteknikCross-sectional area measuring device
US3883798 *Apr 19, 1974May 13, 1975Hoffmann La RocheFree flow resonant cavity measuring apparatus
US4206399 *Mar 27, 1978Jun 3, 1980Bayer AktiengesellschaftApparatus for determining the water content of isotropic materials by means of microwave absorption
US4358731 *May 23, 1980Nov 9, 1982Philip Morris IncorporatedApparatus and method for moisture measurement
US4571544 *Nov 10, 1983Feb 18, 1986Aluminum Company Of AmericaMicrowave examination of semiconductive shields
US4700127 *May 1, 1985Oct 13, 1987Nippon Soken, Inc.Microwave probe and rotary body detecting apparatus using the same
US4781063 *Jan 30, 1987Nov 1, 1988Shigeyoshi OsakiMethod of measuring orientation of sheet or web like material
US5103181 *Oct 5, 1988Apr 7, 1992Den Norske Oljeselskap A. S.Composition monitor and monitoring process using impedance measurements
US5241279 *Mar 27, 1992Aug 31, 1993Alcatel N.V.Microwave measuring apparatus for continuously and without contact measuring the thickness of a thin conducting layer of a running insulating support such as a fiber or a tape
EP0064621A2 *Apr 20, 1982Nov 17, 1982Magyar Tudományos Akadémia Müszaki Fizikai Kutato IntézeteDetection of moving solid or fluid bodies using microwaves
EP0508854A1 *Mar 26, 1992Oct 14, 1992Alcatel N.V.Continuous contact-free thickness measuring device for thin conductive films on an insulating substrate, such as a moving fibre or band
Classifications
U.S. Classification324/636, 324/543, 333/230
International ClassificationG01N22/02, G01N22/00
Cooperative ClassificationG01N22/02
European ClassificationG01N22/02