Deformation induced electromagnetic response of soft and hard PZT under impact loading
Electromagnetic radiation (EMR) from soft and hard PZT under the drop weight impact have been studied. Due to impact the PZT undergoes a deformation wave which causes oscillations of dipoles within the PZT which give rise to electromagnetic radiation. The peak EMR voltage and the average EMR energy...
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| Autor*in: |
Kumar, Amit [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2017 |
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| Rechteinformationen: |
Nutzungsrecht: © 2017 Taylor & Francis Group, LLC 2017 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Ferroelectrics - Philadelphia, Pa. : Taylor & Francis, 1970, 510(2017), 1, Seite 170 |
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| Übergeordnetes Werk: |
volume:510 ; year:2017 ; number:1 ; pages:170 |
| Links: |
|---|
| DOI / URN: |
10.1080/00150193.2017.1328726 |
|---|
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| 520 | |a Electromagnetic radiation (EMR) from soft and hard PZT under the drop weight impact have been studied. Due to impact the PZT undergoes a deformation wave which causes oscillations of dipoles within the PZT which give rise to electromagnetic radiation. The peak EMR voltage and the average EMR energy release rate show a linearly increasing pattern with the height of impact suggesting that these parameters could be used for monitoring excessive deformation from the structures. EMR peak voltage and average EMR energy release rate obtained from the soft PZT SP-5A are 43.42% and 53.12% higher respectively from those obtained from the hard PZT SP-4 owing to the higher resistance offered by the hard PZT to the domain switching. | ||
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| 650 | 4 | |a Electromagnetic radiation (EMR) | |
| 650 | 4 | |a impact loading | |
| 650 | 4 | |a PZT | |
| 650 | 4 | |a Electromagnetic radiation | |
| 650 | 4 | |a Deformation mechanisms | |
| 650 | 4 | |a Switching | |
| 650 | 4 | |a Radiation | |
| 650 | 4 | |a Energy | |
| 650 | 4 | |a Impact loading | |
| 650 | 4 | |a Electric potential | |
| 650 | 4 | |a Energy release rate | |
| 650 | 4 | |a Deformation | |
| 650 | 4 | |a Lead zirconate titanates | |
| 700 | 1 | |a Chauhan, Vishal S |4 oth | |
| 700 | 1 | |a Sharma, Sumeet Kumar |4 oth | |
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10.1080/00150193.2017.1328726 doi PQ20170721 (DE-627)OLC1995051101 (DE-599)GBVOLC1995051101 (PRQ)i1130-636b9146e4e144f6511e858030314b2ff85659f8f6c8cff31aef8b71ed87b6a20 (KEY)0160238120170000510000100170deformationinducedelectromagneticresponseofsoftand DE-627 ger DE-627 rakwb eng 530 620 DNB Kumar, Amit verfasserin aut Deformation induced electromagnetic response of soft and hard PZT under impact loading 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Electromagnetic radiation (EMR) from soft and hard PZT under the drop weight impact have been studied. Due to impact the PZT undergoes a deformation wave which causes oscillations of dipoles within the PZT which give rise to electromagnetic radiation. The peak EMR voltage and the average EMR energy release rate show a linearly increasing pattern with the height of impact suggesting that these parameters could be used for monitoring excessive deformation from the structures. EMR peak voltage and average EMR energy release rate obtained from the soft PZT SP-5A are 43.42% and 53.12% higher respectively from those obtained from the hard PZT SP-4 owing to the higher resistance offered by the hard PZT to the domain switching. Nutzungsrecht: © 2017 Taylor & Francis Group, LLC 2017 Electromagnetic radiation (EMR) impact loading PZT Electromagnetic radiation Deformation mechanisms Switching Radiation Energy Impact loading Electric potential Energy release rate Deformation Lead zirconate titanates Chauhan, Vishal S oth Sharma, Sumeet Kumar oth Kumar, Rajeev oth Enthalten in Ferroelectrics Philadelphia, Pa. : Taylor & Francis, 1970 510(2017), 1, Seite 170 (DE-627)129356948 (DE-600)160137-4 (DE-576)014728990 0015-0193 nnns volume:510 year:2017 number:1 pages:170 http://dx.doi.org/10.1080/00150193.2017.1328726 Volltext http://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1328726 https://search.proquest.com/docview/1915315170 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 510 2017 1 170 |
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10.1080/00150193.2017.1328726 doi PQ20170721 (DE-627)OLC1995051101 (DE-599)GBVOLC1995051101 (PRQ)i1130-636b9146e4e144f6511e858030314b2ff85659f8f6c8cff31aef8b71ed87b6a20 (KEY)0160238120170000510000100170deformationinducedelectromagneticresponseofsoftand DE-627 ger DE-627 rakwb eng 530 620 DNB Kumar, Amit verfasserin aut Deformation induced electromagnetic response of soft and hard PZT under impact loading 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Electromagnetic radiation (EMR) from soft and hard PZT under the drop weight impact have been studied. Due to impact the PZT undergoes a deformation wave which causes oscillations of dipoles within the PZT which give rise to electromagnetic radiation. The peak EMR voltage and the average EMR energy release rate show a linearly increasing pattern with the height of impact suggesting that these parameters could be used for monitoring excessive deformation from the structures. EMR peak voltage and average EMR energy release rate obtained from the soft PZT SP-5A are 43.42% and 53.12% higher respectively from those obtained from the hard PZT SP-4 owing to the higher resistance offered by the hard PZT to the domain switching. Nutzungsrecht: © 2017 Taylor & Francis Group, LLC 2017 Electromagnetic radiation (EMR) impact loading PZT Electromagnetic radiation Deformation mechanisms Switching Radiation Energy Impact loading Electric potential Energy release rate Deformation Lead zirconate titanates Chauhan, Vishal S oth Sharma, Sumeet Kumar oth Kumar, Rajeev oth Enthalten in Ferroelectrics Philadelphia, Pa. : Taylor & Francis, 1970 510(2017), 1, Seite 170 (DE-627)129356948 (DE-600)160137-4 (DE-576)014728990 0015-0193 nnns volume:510 year:2017 number:1 pages:170 http://dx.doi.org/10.1080/00150193.2017.1328726 Volltext http://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1328726 https://search.proquest.com/docview/1915315170 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 510 2017 1 170 |
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Deformation induced electromagnetic response of soft and hard PZT under impact loading |
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| title_full |
Deformation induced electromagnetic response of soft and hard PZT under impact loading |
| author_sort |
Kumar, Amit |
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Ferroelectrics |
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Ferroelectrics |
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eng |
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false |
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500 - Science 600 - Technology |
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2017 |
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170 |
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Kumar, Amit |
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510 |
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530 620 DNB |
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Aufsätze |
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Kumar, Amit |
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10.1080/00150193.2017.1328726 |
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530 620 |
| title_sort |
deformation induced electromagnetic response of soft and hard pzt under impact loading |
| title_auth |
Deformation induced electromagnetic response of soft and hard PZT under impact loading |
| abstract |
Electromagnetic radiation (EMR) from soft and hard PZT under the drop weight impact have been studied. Due to impact the PZT undergoes a deformation wave which causes oscillations of dipoles within the PZT which give rise to electromagnetic radiation. The peak EMR voltage and the average EMR energy release rate show a linearly increasing pattern with the height of impact suggesting that these parameters could be used for monitoring excessive deformation from the structures. EMR peak voltage and average EMR energy release rate obtained from the soft PZT SP-5A are 43.42% and 53.12% higher respectively from those obtained from the hard PZT SP-4 owing to the higher resistance offered by the hard PZT to the domain switching. |
| abstractGer |
Electromagnetic radiation (EMR) from soft and hard PZT under the drop weight impact have been studied. Due to impact the PZT undergoes a deformation wave which causes oscillations of dipoles within the PZT which give rise to electromagnetic radiation. The peak EMR voltage and the average EMR energy release rate show a linearly increasing pattern with the height of impact suggesting that these parameters could be used for monitoring excessive deformation from the structures. EMR peak voltage and average EMR energy release rate obtained from the soft PZT SP-5A are 43.42% and 53.12% higher respectively from those obtained from the hard PZT SP-4 owing to the higher resistance offered by the hard PZT to the domain switching. |
| abstract_unstemmed |
Electromagnetic radiation (EMR) from soft and hard PZT under the drop weight impact have been studied. Due to impact the PZT undergoes a deformation wave which causes oscillations of dipoles within the PZT which give rise to electromagnetic radiation. The peak EMR voltage and the average EMR energy release rate show a linearly increasing pattern with the height of impact suggesting that these parameters could be used for monitoring excessive deformation from the structures. EMR peak voltage and average EMR energy release rate obtained from the soft PZT SP-5A are 43.42% and 53.12% higher respectively from those obtained from the hard PZT SP-4 owing to the higher resistance offered by the hard PZT to the domain switching. |
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| title_short |
Deformation induced electromagnetic response of soft and hard PZT under impact loading |
| url |
http://dx.doi.org/10.1080/00150193.2017.1328726 http://www.tandfonline.com/doi/abs/10.1080/00150193.2017.1328726 https://search.proquest.com/docview/1915315170 |
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false |
| author2 |
Chauhan, Vishal S Sharma, Sumeet Kumar Kumar, Rajeev |
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Chauhan, Vishal S Sharma, Sumeet Kumar Kumar, Rajeev |
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10.1080/00150193.2017.1328726 |
| up_date |
2024-07-03T20:16:10.812Z |
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