The invention relates to the technical field of ultrasonic inspection, specifically relating to an electromagnetic ultrasonic double-wave transducer.
In the field of ultrasonic inspection, it is sometimes necessary to use two modes of waves to accurately detect a part for inspection for certain material properties, dimensions, or defects. For example, in the detection of the nodularity of spheroidal graphite cast iron, if there is only one mode of waves, it is not easy to distinguish whether the change in the time-of-flight is from a change in the thickness of the sample or from a change in the speed of the ultrasonic wave itself, which greatly affects the effectiveness of the inspection. For example, in the assessment of the tensile force of the bolt, if only one mode of ultrasonic wave is adopted, it cannot be known whether the time-of-flight of the ultrasonic wave is from the change of the part's dimension or the change of the speed of the ultrasonic wave caused by the tensile stress of the bolt. Thus, the bolt tension cannot be detected by an ultrasonic method.
In order to generate ultrasonic waves of two different modes, the open literature 1 (NDT&E International 42 (2009) 164-169) mentioned that the ultrasonic longitudinal wave generates mode-converted transverse wave on the reflection bottom surface of the part to be measured by employing a specially designed piezoelectric ultrasonic transducer; the open literature 2 (Ultrasonics 54 (2014) 914-920) mentions that an electromagnetic ultrasonic transverse wave transducer generates mode-converted longitudinal wave at the reflection bottom of the part to be tested by using a high-power source for excitation and a multiple averaging method; the open literature 3 (Vol. 17 (1996) No. 6 662-665, Chinese Journal of Scientific Instrument) mentions that the ultrasonic longitudinal waves and transverse waves are respectively generated in the testing part by adopting two piezoelectric transducers in combination; the open literature 4 (U.S. Pat. No. 8,511,165B2) mentions the use of a piezoelectric transducer in combination with an electromagnetic ultrasonic transducer to generate longitudinal and transverse waves, respectively, on the surface of a testing part.
None of the methods in the above open literature can generate both longitudinal wave and transverse wave on the surface of the part to be inspected, causing errors in high-precision inspection, particularly in bolt tension inspection. The piezoelectric transducers referred to in the open literature 1 to 4 need to take the influence of the wedges and the couplant on the propagation time of the ultrasonic wave during the forward and backward propagation of the ultrasonic wave from the piezoelectric wafer to the surface of the part to be tested. Neither of the electromagnetic ultrasonic transducers described in the open literature 2 and 4 can generate ultrasonic longitudinal wave on the surface of a testing part.
Based on the problems in the prior art, the invention aims at providing an electromagnetic ultrasonic double-wave transducer, which can simultaneously generate longitudinal wave and transverse wave on the surface of a testing part.
Based on the above problems, the invention provides a technical solution:
An electromagnetic ultrasonic double-wave transducer, comprising a shell, and a permanent magnet assembly, a coil, a shielding layer, and a wire which are provided in said shell.
Said permanent magnet assembly comprises a first permanent magnet and a second permanent magnet sleeved on the first permanent magnet. The magnetizing directions of the first permanent magnet and the second permanent magnet are perpendicular to the bottom of said shell, and the magnetic field directions of said first permanent magnet and the second permanent magnet are opposite; a non-conducting non-magnetic bushing material is provided between said first permanent magnet and said second permanent magnet, and upper end faces of said first permanent magnet and said second permanent magnet realize magnetic circuit closing by means of a magnetic circuit closing element.
Said coil is fixed on the bottom of said shell and is located below said first permanent magnet. Said shielding layer is provided between the lower end of said first permanent magnet and said coil and below said second permanent magnet. One end of said wire is connected to said coil, and the other end is connected to power supply and signal plug.
In one embodiment, said first permanent magnet is cylindrical while said second permanent magnet is annular.
In one embodiment, the inner diameter of said second permanent magnet is 1-15 mm larger than the outer diameter of said first permanent magnet.
In one embodiment, the lower end faces of said first permanent magnet and said second permanent magnet have a height difference from −3 mm to 3 mm.
In one embodiment, said coil is helical, and the outer diameter thereof is larger than the outer diameter of said first permanent magnet and smaller than the inner diameter of said second permanent magnet.
In one embodiment, the non-conductive material is filled between said coil and said shielding layer, and the non-conducting non-magnetic material is filled between said permanent magnet assembly and said shell.
In one embodiment, said shell includes a shell body and a wear plate disposed at the lower end of said shell body.
Based on the above problems, the second technical solution provided by the invention is as follows:
An electromagnetic ultrasonic double-wave transducer, comprising a shell, and a permanent magnet assembly, a coil, a shielding layer, and a wire which are provided in said shell. Said coil is fixed on the bottom of said shell and is located below said permanent magnet assembly; said shielding layer is arranged between said permanent magnet assembly and said coil; one end of said wire is connected to said coil while the other end thereof is connected to power and signal plug; said permanent magnet assembly comprises a third permanent magnet and a fourth permanent magnet wherein the fourth permanent magnet are arranged side by side with said third permanent magnet and located on two sides of the width direction of said third permanent magnet, and said fourth permanent magnet and said third permanent magnet are arranged at intervals and said intervals are made of non-conducting non-magnetic bushing material; the upper end faces of said third permanent magnet and said fourth permanent magnet realize magnetic circuit closing by means of a magnetic circuit closing element.
In one embodiment, the cross sections of said third permanent magnet and said fourth permanent magnet are rectangular.
In one embodiment, said coil is butterfly shaped.
In one embodiment, the non-conductive material is filled between said coil and said shielding layer, and the non-conducting non-magnet-conduction material is filled between said permanent magnet assembly and said shell.
In one embodiment, said shell includes a shell body and a wear plate disposed at the lower end of said shell body.
Compared with the prior art, the invention has following advantages;
By adopting the technical solution of the invention, the ultrasonic transducer can simultaneously excite longitudinal waves and transverse waves on the surface of a testing part, and the two modes of ultrasonic waves are used for detecting physical quantities such as material properties like elastic modulus of materials, defects, length, stress and the like, thereby the measurement error caused by the time delay of the piezoelectric ultrasonic wedge and the coupling agent is avoided, the detection error possibly caused by the mode conversion of the ultrasonic waves is also avoided, and the detection precision is improved.
In order to more clearly illustrate the technical solutions of the embodiments of the invention, the drawings required to be used in the description of the embodiments are briefly introduced below, the drawings in the description are only some embodiments of the invention, and it is obvious for those skilled in the art that other drawings can be obtained according to the drawings without creative efforts.
Wherein:
The above-described solution is further illustrated below with reference to specific embodiments. It should be understood that these embodiments are for illustrative purposes and are not intended to limit the scope of the invention. The conditions used in the embodiments may be further adjusted according to the conditions of the particular manufacturer, and the conditions not specified are generally conditions used in routine experiments.
As is shown in
The permanent magnet assembly comprises a first permanent magnet 2 and a second permanent magnet 3 sleeved on the first permanent magnet 2. The magnetizing directions of the first permanent magnet 2 and the second permanent magnet 3 are perpendicular to the bottom of the shell 1, and the magnetic field directions of the first permanent magnet 2 and the second permanent magnet 3 are opposite. A non-conducting non-magnetic bushing material 9 is provided between the first permanent magnet 2 and the second permanent magnet 3, and upper end faces of the first permanent magnet 2 and the second permanent magnet 3 realize magnetic circuit closing by means of a magnetic circuit closing element 8.
Said coil 4 is fixed on the bottom of said shell 1 and is located below said first permanent magnet 2. Said shielding layer 5 is provided between the lower end of said first permanent magnet 2 and said coil 4 and below said second permanent magnet 3. One end of said wire 6 is connected to said coil 4, and the other end is connected to a power supply and signal plug 7.
In this embodiment, the magnetic circuit closing element 8 is made of mild steel or ferrite with a thickness greater than 3 mm. The non-conducting non-magnetic bushing material 9 is made of plastic, rubber or polymer material, such as bakelite.
The inner diameter of said second permanent magnet 3 is 1-15 mm larger than the outer diameter of said first permanent magnet 2, and said coil 4 is helical, and the outer diameter thereof is larger than the outer diameter of said first permanent magnet 2 and smaller than the inner diameter of said second permanent magnet 3. The lower end face of the first permanent magnet 2 can be flush with that of the second permanent magnet 3, and they also can have a height difference of less than 3 mm, which means that the lower end face of the first permanent magnet 2 is located above that of the second permanent magnet 3, or is located below that of the second permanent magnet 3.
In this embodiment, the shielding layer 5 is a highly conductive copper sheet or silver sheet, and is attached to the lower ends of the first permanent magnet 2 and the second permanent magnet 3.
In order to further optimize the implementation effect of the invention, the non-conductive material 10 is filled between said coil 4 and said shielding layer 5, such as air, resin and non-conductive soft magnetic material; the non-conducting non-magnetic material is filled between said permanent magnet assembly and said shell 1, i.e., epoxy resin.
In this embodiment, said coil 4 is made of double-layer PCB board or wound by enameled wire.
In this embodiment, said shell 1 includes a shell body 1-1 and a wear plate 1-2 disposed at the lower end of said shell body 1-1; the wear plate 1-2 is made of ceramic wafer or epoxy plate and the shell body 1-1 is made of stainless steel, aluminum alloy or red copper material; the power supply and signal plug 7 is fixed at the upper part of the shell body 1-1.
As is shown in
In this embodiment, the cross sections of said third permanent magnet 12 and said fourth permanent magnet 13 are rectangular and said coil 4 is butterfly shaped.
In the implementation, the first permanent magnet 2, the second permanent magnet 3, the third permanent magnet 12 and the fourth permanent magnet 13 are all made of NdFeB materials.
The electromagnetic ultrasonic transducer can simultaneously excite vertical downward-transmitted ultrasonic transverse waves and ultrasonic longitudinal waves on the near surface of a conductive or magnetic testing part such as low-carbon steel, aluminum alloy and the like, and the amplitude of the longitudinal waves excited by said electromagnetic ultrasonic transducer can reach 20% to 30% of the transverse waves at most in a test with a matched instrument. While the conventional electromagnetic ultrasonic transducer can hardly excite longitudinal wave.
For example, the Young's modulus and the Poisson's ratio of isotropic materials were detected by using the electromagnetic ultrasonic double-wave transducer of embodiment 1.
In isotropic materials, the elasticity modulus E and Poisson's ratio V are related to the velocity of the longitudinal wave Cl and the transverse wave CS as follows:
where T is defined as T≡Cl/CS, ρ) is the density, and taken 7.87×103 kg/m3 for 20 #carbon steel.
Therefore, the Young's modulus and the Poisson's ratio of the material can be estimated by detecting the longitudinal wave velocity, the transverse wave velocity and the density of the material.
A hand-held high-power ultrasonic testing instrument PREMAT-HS200 manufactured by Suzhou Phaserise Technology Co., Ltd. is used as an electromagnetic ultrasonic pulser/receiver equipped with the electromagnetic ultrasonic double-wave transducer of the invention. The testing part is selected from a CSK-II A standard sample according to JB/T 4730-2005 standard. The sample dimension is 300 mm long, 60 mm wide and 40 mm in height The electromagnetic ultrasonic transducer is placed in the middle of the upper surface of the sample to be tested, and is 170 mm away from the left edge of the sample, and 35 mm away from the upper edge. The test frequency is 4 MHz, the excitation voltage 1200Vpp, the display delay 10 μs, the sampling time 80 μs, the sampling speed 100 MS/s, and the repetition rate 200 Hz. The test data for the automatic gain is shown in
Calculations from equations (1) and (2) using the data in table 1 lead to:
E=2.1226×1011 Pa (3)
v=0.285 (4)
The results are very close to the nominal value of the sample.
Table 1: Time-of-flight of longitudinal wave and transverse wave excited on surface of the testing part.
The transducer of the invention can be used for accurate detection of bolt tension. According to some open literature, the bolt stress is a linear function of the ratio of longitudinal wave time-of-flight and transverse wave time-of-flight.
For the bolt with calibrated material parameters, the tensile stress applied to the bolt can be calculated as long as TOFS and TOFl can be accurately measured. The transducer used by the invention can simultaneously excite longitudinal waves and transverse waves on the inspection surface end of the bolt.
For instance, Young's modulus and the Poisson's ratio of isotropic materials were measured by using the electromagnetic ultrasonic double-wave transducer of embodiment 2.
After selecting the same sample and measurement parameters as in embodiment 1, The
The above embodiments are provided only for illustrating the technical concepts and features of the invention, and the purpose of the invention is to provide those skilled in the art with the understanding of the invention and to implement the invention, and not to limit the scope of the invention. All equivalent changes and modifications made according to the spirit of the invention should all fall within the protection scope of the invention.
Number | Date | Country | Kind |
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201810893704.4 | Aug 2018 | CN | national |
Filing Document | Filing Date | Country | Kind |
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PCT/CN2018/112179 | 10/26/2018 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2020/029435 | 2/13/2020 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
4063157 | Lorenzi | Dec 1977 | A |
4296486 | Vasile | Oct 1981 | A |
4395913 | Peterson | Aug 1983 | A |
5050703 | Graff | Sep 1991 | A |
5148414 | Graff | Sep 1992 | A |
5164921 | Graff | Nov 1992 | A |
5277751 | Ogle | Jan 1994 | A |
5689070 | Clark | Nov 1997 | A |
5811682 | Ohtani | Sep 1998 | A |
5900793 | Katznelson | May 1999 | A |
6109108 | Ohtani | Aug 2000 | A |
6125706 | Buttram | Oct 2000 | A |
6176132 | MacLauchlan | Jan 2001 | B1 |
6640635 | Nakatsuka | Nov 2003 | B2 |
6766694 | Hubschen | Jul 2004 | B2 |
7697375 | Reiderman | Apr 2010 | B2 |
7726193 | Reiderman | Jun 2010 | B2 |
8037764 | Kroning | Oct 2011 | B2 |
8037765 | Reiderman | Oct 2011 | B2 |
8511165 | Lopez Jauregui | Aug 2013 | B2 |
8596129 | Niese | Dec 2013 | B2 |
8789422 | Ege | Jul 2014 | B2 |
9983073 | May | May 2018 | B2 |
10408796 | Bondurant | Sep 2019 | B2 |
10436018 | Kouchmeshky | Oct 2019 | B2 |
10502714 | Ren | Dec 2019 | B2 |
10537916 | Cegla | Jan 2020 | B2 |
10591443 | Lopatin | Mar 2020 | B2 |
11385115 | Walaszek | Jul 2022 | B2 |
11421986 | Shen | Aug 2022 | B2 |
11442042 | Stanton | Sep 2022 | B2 |
11493581 | Han | Nov 2022 | B2 |
20030011451 | Katznelson | Jan 2003 | A1 |
20110259108 | Ege | Oct 2011 | A1 |
20120103097 | Lopez Jauregui | May 2012 | A1 |
20120240681 | Lopez Jauregui | Sep 2012 | A1 |
20170299554 | Bondurant et al. | Oct 2017 | A1 |
20170333946 | Cegla | Nov 2017 | A1 |
20180356369 | Tamura | Dec 2018 | A1 |
20200393417 | Lopez Jauregui | Dec 2020 | A1 |
20210341432 | Ren | Nov 2021 | A1 |
Number | Date | Country |
---|---|---|
104820024 | Aug 2015 | CN |
204854670 | Dec 2015 | CN |
105975728 | Jun 2016 | CN |
107064311 | Aug 2017 | CN |
107206424 | Sep 2017 | CN |
108375433 | Aug 2018 | CN |
2000146923 | May 2000 | JP |
2010025812 | Feb 2010 | JP |
2014102157 | Jun 2014 | JP |
Number | Date | Country | |
---|---|---|---|
20210293639 A1 | Sep 2021 | US |