Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting
Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation i...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Tao, Z. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2016 |
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| Schlagwörter: |
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| Anmerkung: |
© The Society for Experimental Mechanics, Inc. 2016 |
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| Übergeordnetes Werk: |
Enthalten in: Experimental techniques - Cham : Springer International Publishing, 1975, 40(2016), 6 vom: 10. Aug., Seite 1539-1547 |
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| Übergeordnetes Werk: |
volume:40 ; year:2016 ; number:6 ; day:10 ; month:08 ; pages:1539-1547 |
| Links: |
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| DOI / URN: |
10.1007/s40799-016-0146-1 |
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| Katalog-ID: |
SPR037809865 |
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| 520 | |a Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. | ||
| 650 | 4 | |a Nondestructive testing |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Permanent magnet |7 (dpeaa)DE-He213 | |
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| 700 | 1 | |a Wang, X. |4 aut | |
| 700 | 1 | |a Chen, X. |4 aut | |
| 700 | 1 | |a Na, X. |4 aut | |
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10.1007/s40799-016-0146-1 doi (DE-627)SPR037809865 (SPR)s40799-016-0146-1-e DE-627 ger DE-627 rakwb eng Tao, Z. verfasserin aut Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Society for Experimental Mechanics, Inc. 2016 Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. Nondestructive testing (dpeaa)DE-He213 Permanent magnet (dpeaa)DE-He213 Magnetostatic force (dpeaa)DE-He213 Wang, X. aut Chen, X. aut Na, X. aut Enthalten in Experimental techniques Cham : Springer International Publishing, 1975 40(2016), 6 vom: 10. Aug., Seite 1539-1547 (DE-627)500635854 (DE-600)2205019-X 1747-1567 nnns volume:40 year:2016 number:6 day:10 month:08 pages:1539-1547 https://dx.doi.org/10.1007/s40799-016-0146-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2016 6 10 08 1539-1547 |
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10.1007/s40799-016-0146-1 doi (DE-627)SPR037809865 (SPR)s40799-016-0146-1-e DE-627 ger DE-627 rakwb eng Tao, Z. verfasserin aut Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Society for Experimental Mechanics, Inc. 2016 Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. Nondestructive testing (dpeaa)DE-He213 Permanent magnet (dpeaa)DE-He213 Magnetostatic force (dpeaa)DE-He213 Wang, X. aut Chen, X. aut Na, X. aut Enthalten in Experimental techniques Cham : Springer International Publishing, 1975 40(2016), 6 vom: 10. Aug., Seite 1539-1547 (DE-627)500635854 (DE-600)2205019-X 1747-1567 nnns volume:40 year:2016 number:6 day:10 month:08 pages:1539-1547 https://dx.doi.org/10.1007/s40799-016-0146-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2016 6 10 08 1539-1547 |
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10.1007/s40799-016-0146-1 doi (DE-627)SPR037809865 (SPR)s40799-016-0146-1-e DE-627 ger DE-627 rakwb eng Tao, Z. verfasserin aut Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Society for Experimental Mechanics, Inc. 2016 Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. Nondestructive testing (dpeaa)DE-He213 Permanent magnet (dpeaa)DE-He213 Magnetostatic force (dpeaa)DE-He213 Wang, X. aut Chen, X. aut Na, X. aut Enthalten in Experimental techniques Cham : Springer International Publishing, 1975 40(2016), 6 vom: 10. Aug., Seite 1539-1547 (DE-627)500635854 (DE-600)2205019-X 1747-1567 nnns volume:40 year:2016 number:6 day:10 month:08 pages:1539-1547 https://dx.doi.org/10.1007/s40799-016-0146-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2016 6 10 08 1539-1547 |
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10.1007/s40799-016-0146-1 doi (DE-627)SPR037809865 (SPR)s40799-016-0146-1-e DE-627 ger DE-627 rakwb eng Tao, Z. verfasserin aut Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Society for Experimental Mechanics, Inc. 2016 Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. Nondestructive testing (dpeaa)DE-He213 Permanent magnet (dpeaa)DE-He213 Magnetostatic force (dpeaa)DE-He213 Wang, X. aut Chen, X. aut Na, X. aut Enthalten in Experimental techniques Cham : Springer International Publishing, 1975 40(2016), 6 vom: 10. Aug., Seite 1539-1547 (DE-627)500635854 (DE-600)2205019-X 1747-1567 nnns volume:40 year:2016 number:6 day:10 month:08 pages:1539-1547 https://dx.doi.org/10.1007/s40799-016-0146-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2016 6 10 08 1539-1547 |
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10.1007/s40799-016-0146-1 doi (DE-627)SPR037809865 (SPR)s40799-016-0146-1-e DE-627 ger DE-627 rakwb eng Tao, Z. verfasserin aut Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Society for Experimental Mechanics, Inc. 2016 Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. Nondestructive testing (dpeaa)DE-He213 Permanent magnet (dpeaa)DE-He213 Magnetostatic force (dpeaa)DE-He213 Wang, X. aut Chen, X. aut Na, X. aut Enthalten in Experimental techniques Cham : Springer International Publishing, 1975 40(2016), 6 vom: 10. Aug., Seite 1539-1547 (DE-627)500635854 (DE-600)2205019-X 1747-1567 nnns volume:40 year:2016 number:6 day:10 month:08 pages:1539-1547 https://dx.doi.org/10.1007/s40799-016-0146-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2016 6 10 08 1539-1547 |
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Tao, Z. |
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Tao, Z. misc Nondestructive testing misc Permanent magnet misc Magnetostatic force Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting |
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Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting Nondestructive testing (dpeaa)DE-He213 Permanent magnet (dpeaa)DE-He213 Magnetostatic force (dpeaa)DE-He213 |
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Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting |
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Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting |
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theory of magnetostatic force inspection method for monitoring the oscillation marks of continuous casting |
| title_auth |
Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting |
| abstract |
Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. © The Society for Experimental Mechanics, Inc. 2016 |
| abstractGer |
Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. © The Society for Experimental Mechanics, Inc. 2016 |
| abstract_unstemmed |
Abstract We report an investigation of magnetostatic force of a permanent magnet passing by casting slab in order to monitor oscillation marks on its surface. This problem represents a highly simplified yet enlightening version called magnetostatic force inspection method (MFIM). Our investigation is a combination of analytic theory, numerical simulation and experimental validation [1]. The method allows a prediction of the relationship between profile of the oscillation marks and the change in magnetostatic force. We test our predictions by performing a series of experiments and numerical simulation to overcome difficulty inherent to the analytic theory. We conclude that MFIM has ability of capturing the characteristics of oscillation marks although a refinement of responding theory is necessary to reduce the discrepancy to the predictions. The present results can serve as a prototype for research on magnetostatic inspection. This paper formulates the MFIM through computing the reaction force of the ferromagnetic material. The magnetic field of the small cubic permanent magnet is modeled by an exponential function together with Gauss distribution possibility density function and this approach makes magnetostatic force by various ferromagnetic oscillation marks solved analytically. Cases of regular profile, triangular, rectangular and circular mimicking marks, provide the key scaling laws of the method and illustrate relation between magnetostatic force and the geometric properties of oscillation marks. It provides a theoretical framework for the prediction of the sensitivity of MFIM in laboratory experiments and implementation in industrial practice. © The Society for Experimental Mechanics, Inc. 2016 |
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Theory of Magnetostatic Force Inspection Method for Monitoring the Oscillation Marks of Continuous Casting |
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https://dx.doi.org/10.1007/s40799-016-0146-1 |
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Wang, X. Chen, X. Na, X. |
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10.1007/s40799-016-0146-1 |
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|
| score |
7.401043 |