Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity
Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very eff...
Ausführliche Beschreibung
Autor*in: |
Yang, H. [verfasserIn] |
---|
Format: |
Artikel |
---|---|
Sprache: |
Englisch |
Erschienen: |
2006 |
---|
Schlagwörter: |
---|
Anmerkung: |
© Society for Experimental Mechanics 2006 |
---|
Übergeordnetes Werk: |
Enthalten in: Experimental mechanics - Kluwer Academic Publishers, 1961, 46(2006), 5 vom: 25. Juli, Seite 619-626 |
---|---|
Übergeordnetes Werk: |
volume:46 ; year:2006 ; number:5 ; day:25 ; month:07 ; pages:619-626 |
Links: |
---|
DOI / URN: |
10.1007/s11340-006-9112-7 |
---|
Katalog-ID: |
OLC2058173465 |
---|
LEADER | 01000caa a22002652 4500 | ||
---|---|---|---|
001 | OLC2058173465 | ||
003 | DE-627 | ||
005 | 20230504082721.0 | ||
007 | tu | ||
008 | 200819s2006 xx ||||| 00| ||eng c | ||
024 | 7 | |a 10.1007/s11340-006-9112-7 |2 doi | |
035 | |a (DE-627)OLC2058173465 | ||
035 | |a (DE-He213)s11340-006-9112-7-p | ||
040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
041 | |a eng | ||
082 | 0 | 4 | |a 690 |q VZ |
100 | 1 | |a Yang, H. |e verfasserin |4 aut | |
245 | 1 | 0 | |a Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity |
264 | 1 | |c 2006 | |
336 | |a Text |b txt |2 rdacontent | ||
337 | |a ohne Hilfsmittel zu benutzen |b n |2 rdamedia | ||
338 | |a Band |b nc |2 rdacarrier | ||
500 | |a © Society for Experimental Mechanics 2006 | ||
520 | |a Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. | ||
650 | 4 | |a Three-dimensional photoelasticity | |
650 | 4 | |a Fourier Polarimetry | |
650 | 4 | |a Tomographic photoelasticity | |
650 | 4 | |a Integrated photoelasticity | |
700 | 1 | |a Gibson, S. |4 aut | |
700 | 1 | |a Tomlinson, R. A. |4 aut | |
773 | 0 | 8 | |i Enthalten in |t Experimental mechanics |d Kluwer Academic Publishers, 1961 |g 46(2006), 5 vom: 25. Juli, Seite 619-626 |w (DE-627)129593990 |w (DE-600)240480-1 |w (DE-576)015086852 |x 0014-4851 |7 nnns |
773 | 1 | 8 | |g volume:46 |g year:2006 |g number:5 |g day:25 |g month:07 |g pages:619-626 |
856 | 4 | 1 | |u https://doi.org/10.1007/s11340-006-9112-7 |z lizenzpflichtig |3 Volltext |
912 | |a GBV_USEFLAG_A | ||
912 | |a SYSFLAG_A | ||
912 | |a GBV_OLC | ||
912 | |a SSG-OLC-UMW | ||
912 | |a SSG-OLC-ARC | ||
912 | |a SSG-OLC-TEC | ||
912 | |a SSG-OLC-PHY | ||
912 | |a GBV_ILN_23 | ||
912 | |a GBV_ILN_62 | ||
912 | |a GBV_ILN_70 | ||
912 | |a GBV_ILN_2020 | ||
912 | |a GBV_ILN_2057 | ||
912 | |a GBV_ILN_4317 | ||
912 | |a GBV_ILN_4700 | ||
951 | |a AR | ||
952 | |d 46 |j 2006 |e 5 |b 25 |c 07 |h 619-626 |
author_variant |
h y hy s g sg r a t ra rat |
---|---|
matchkey_str |
article:00144851:2006----::mrvmnofuiroaierfrplctosnoor |
hierarchy_sort_str |
2006 |
publishDate |
2006 |
allfields |
10.1007/s11340-006-9112-7 doi (DE-627)OLC2058173465 (DE-He213)s11340-006-9112-7-p DE-627 ger DE-627 rakwb eng 690 VZ Yang, H. verfasserin aut Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Society for Experimental Mechanics 2006 Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. Three-dimensional photoelasticity Fourier Polarimetry Tomographic photoelasticity Integrated photoelasticity Gibson, S. aut Tomlinson, R. A. aut Enthalten in Experimental mechanics Kluwer Academic Publishers, 1961 46(2006), 5 vom: 25. Juli, Seite 619-626 (DE-627)129593990 (DE-600)240480-1 (DE-576)015086852 0014-4851 nnns volume:46 year:2006 number:5 day:25 month:07 pages:619-626 https://doi.org/10.1007/s11340-006-9112-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-UMW SSG-OLC-ARC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_23 GBV_ILN_62 GBV_ILN_70 GBV_ILN_2020 GBV_ILN_2057 GBV_ILN_4317 GBV_ILN_4700 AR 46 2006 5 25 07 619-626 |
spelling |
10.1007/s11340-006-9112-7 doi (DE-627)OLC2058173465 (DE-He213)s11340-006-9112-7-p DE-627 ger DE-627 rakwb eng 690 VZ Yang, H. verfasserin aut Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Society for Experimental Mechanics 2006 Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. Three-dimensional photoelasticity Fourier Polarimetry Tomographic photoelasticity Integrated photoelasticity Gibson, S. aut Tomlinson, R. A. aut Enthalten in Experimental mechanics Kluwer Academic Publishers, 1961 46(2006), 5 vom: 25. Juli, Seite 619-626 (DE-627)129593990 (DE-600)240480-1 (DE-576)015086852 0014-4851 nnns volume:46 year:2006 number:5 day:25 month:07 pages:619-626 https://doi.org/10.1007/s11340-006-9112-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-UMW SSG-OLC-ARC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_23 GBV_ILN_62 GBV_ILN_70 GBV_ILN_2020 GBV_ILN_2057 GBV_ILN_4317 GBV_ILN_4700 AR 46 2006 5 25 07 619-626 |
allfields_unstemmed |
10.1007/s11340-006-9112-7 doi (DE-627)OLC2058173465 (DE-He213)s11340-006-9112-7-p DE-627 ger DE-627 rakwb eng 690 VZ Yang, H. verfasserin aut Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Society for Experimental Mechanics 2006 Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. Three-dimensional photoelasticity Fourier Polarimetry Tomographic photoelasticity Integrated photoelasticity Gibson, S. aut Tomlinson, R. A. aut Enthalten in Experimental mechanics Kluwer Academic Publishers, 1961 46(2006), 5 vom: 25. Juli, Seite 619-626 (DE-627)129593990 (DE-600)240480-1 (DE-576)015086852 0014-4851 nnns volume:46 year:2006 number:5 day:25 month:07 pages:619-626 https://doi.org/10.1007/s11340-006-9112-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-UMW SSG-OLC-ARC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_23 GBV_ILN_62 GBV_ILN_70 GBV_ILN_2020 GBV_ILN_2057 GBV_ILN_4317 GBV_ILN_4700 AR 46 2006 5 25 07 619-626 |
allfieldsGer |
10.1007/s11340-006-9112-7 doi (DE-627)OLC2058173465 (DE-He213)s11340-006-9112-7-p DE-627 ger DE-627 rakwb eng 690 VZ Yang, H. verfasserin aut Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Society for Experimental Mechanics 2006 Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. Three-dimensional photoelasticity Fourier Polarimetry Tomographic photoelasticity Integrated photoelasticity Gibson, S. aut Tomlinson, R. A. aut Enthalten in Experimental mechanics Kluwer Academic Publishers, 1961 46(2006), 5 vom: 25. Juli, Seite 619-626 (DE-627)129593990 (DE-600)240480-1 (DE-576)015086852 0014-4851 nnns volume:46 year:2006 number:5 day:25 month:07 pages:619-626 https://doi.org/10.1007/s11340-006-9112-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-UMW SSG-OLC-ARC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_23 GBV_ILN_62 GBV_ILN_70 GBV_ILN_2020 GBV_ILN_2057 GBV_ILN_4317 GBV_ILN_4700 AR 46 2006 5 25 07 619-626 |
allfieldsSound |
10.1007/s11340-006-9112-7 doi (DE-627)OLC2058173465 (DE-He213)s11340-006-9112-7-p DE-627 ger DE-627 rakwb eng 690 VZ Yang, H. verfasserin aut Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Society for Experimental Mechanics 2006 Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. Three-dimensional photoelasticity Fourier Polarimetry Tomographic photoelasticity Integrated photoelasticity Gibson, S. aut Tomlinson, R. A. aut Enthalten in Experimental mechanics Kluwer Academic Publishers, 1961 46(2006), 5 vom: 25. Juli, Seite 619-626 (DE-627)129593990 (DE-600)240480-1 (DE-576)015086852 0014-4851 nnns volume:46 year:2006 number:5 day:25 month:07 pages:619-626 https://doi.org/10.1007/s11340-006-9112-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-UMW SSG-OLC-ARC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_23 GBV_ILN_62 GBV_ILN_70 GBV_ILN_2020 GBV_ILN_2057 GBV_ILN_4317 GBV_ILN_4700 AR 46 2006 5 25 07 619-626 |
language |
English |
source |
Enthalten in Experimental mechanics 46(2006), 5 vom: 25. Juli, Seite 619-626 volume:46 year:2006 number:5 day:25 month:07 pages:619-626 |
sourceStr |
Enthalten in Experimental mechanics 46(2006), 5 vom: 25. Juli, Seite 619-626 volume:46 year:2006 number:5 day:25 month:07 pages:619-626 |
format_phy_str_mv |
Article |
institution |
findex.gbv.de |
topic_facet |
Three-dimensional photoelasticity Fourier Polarimetry Tomographic photoelasticity Integrated photoelasticity |
dewey-raw |
690 |
isfreeaccess_bool |
false |
container_title |
Experimental mechanics |
authorswithroles_txt_mv |
Yang, H. @@aut@@ Gibson, S. @@aut@@ Tomlinson, R. A. @@aut@@ |
publishDateDaySort_date |
2006-07-25T00:00:00Z |
hierarchy_top_id |
129593990 |
dewey-sort |
3690 |
id |
OLC2058173465 |
language_de |
englisch |
fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2058173465</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230504082721.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s2006 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11340-006-9112-7</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2058173465</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s11340-006-9112-7-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">690</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Yang, H.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2006</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Society for Experimental Mechanics 2006</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Three-dimensional photoelasticity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Fourier Polarimetry</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Tomographic photoelasticity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Integrated photoelasticity</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gibson, S.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tomlinson, R. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Experimental mechanics</subfield><subfield code="d">Kluwer Academic Publishers, 1961</subfield><subfield code="g">46(2006), 5 vom: 25. Juli, Seite 619-626</subfield><subfield code="w">(DE-627)129593990</subfield><subfield code="w">(DE-600)240480-1</subfield><subfield code="w">(DE-576)015086852</subfield><subfield code="x">0014-4851</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:46</subfield><subfield code="g">year:2006</subfield><subfield code="g">number:5</subfield><subfield code="g">day:25</subfield><subfield code="g">month:07</subfield><subfield code="g">pages:619-626</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s11340-006-9112-7</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-UMW</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-ARC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2057</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4317</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">46</subfield><subfield code="j">2006</subfield><subfield code="e">5</subfield><subfield code="b">25</subfield><subfield code="c">07</subfield><subfield code="h">619-626</subfield></datafield></record></collection>
|
author |
Yang, H. |
spellingShingle |
Yang, H. ddc 690 misc Three-dimensional photoelasticity misc Fourier Polarimetry misc Tomographic photoelasticity misc Integrated photoelasticity Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity |
authorStr |
Yang, H. |
ppnlink_with_tag_str_mv |
@@773@@(DE-627)129593990 |
format |
Article |
dewey-ones |
690 - Buildings |
delete_txt_mv |
keep |
author_role |
aut aut aut |
collection |
OLC |
remote_str |
false |
illustrated |
Not Illustrated |
issn |
0014-4851 |
topic_title |
690 VZ Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity Three-dimensional photoelasticity Fourier Polarimetry Tomographic photoelasticity Integrated photoelasticity |
topic |
ddc 690 misc Three-dimensional photoelasticity misc Fourier Polarimetry misc Tomographic photoelasticity misc Integrated photoelasticity |
topic_unstemmed |
ddc 690 misc Three-dimensional photoelasticity misc Fourier Polarimetry misc Tomographic photoelasticity misc Integrated photoelasticity |
topic_browse |
ddc 690 misc Three-dimensional photoelasticity misc Fourier Polarimetry misc Tomographic photoelasticity misc Integrated photoelasticity |
format_facet |
Aufsätze Gedruckte Aufsätze |
format_main_str_mv |
Text Zeitschrift/Artikel |
carriertype_str_mv |
nc |
hierarchy_parent_title |
Experimental mechanics |
hierarchy_parent_id |
129593990 |
dewey-tens |
690 - Building & construction |
hierarchy_top_title |
Experimental mechanics |
isfreeaccess_txt |
false |
familylinks_str_mv |
(DE-627)129593990 (DE-600)240480-1 (DE-576)015086852 |
title |
Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity |
ctrlnum |
(DE-627)OLC2058173465 (DE-He213)s11340-006-9112-7-p |
title_full |
Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity |
author_sort |
Yang, H. |
journal |
Experimental mechanics |
journalStr |
Experimental mechanics |
lang_code |
eng |
isOA_bool |
false |
dewey-hundreds |
600 - Technology |
recordtype |
marc |
publishDateSort |
2006 |
contenttype_str_mv |
txt |
container_start_page |
619 |
author_browse |
Yang, H. Gibson, S. Tomlinson, R. A. |
container_volume |
46 |
class |
690 VZ |
format_se |
Aufsätze |
author-letter |
Yang, H. |
doi_str_mv |
10.1007/s11340-006-9112-7 |
dewey-full |
690 |
title_sort |
improvement of fourier polarimetry for applications in tomographic photoelasticity |
title_auth |
Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity |
abstract |
Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. © Society for Experimental Mechanics 2006 |
abstractGer |
Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. © Society for Experimental Mechanics 2006 |
abstract_unstemmed |
Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested. © Society for Experimental Mechanics 2006 |
collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-UMW SSG-OLC-ARC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_23 GBV_ILN_62 GBV_ILN_70 GBV_ILN_2020 GBV_ILN_2057 GBV_ILN_4317 GBV_ILN_4700 |
container_issue |
5 |
title_short |
Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity |
url |
https://doi.org/10.1007/s11340-006-9112-7 |
remote_bool |
false |
author2 |
Gibson, S. Tomlinson, R. A. |
author2Str |
Gibson, S. Tomlinson, R. A. |
ppnlink |
129593990 |
mediatype_str_mv |
n |
isOA_txt |
false |
hochschulschrift_bool |
false |
doi_str |
10.1007/s11340-006-9112-7 |
up_date |
2024-07-03T17:58:30.338Z |
_version_ |
1803581663833227264 |
fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2058173465</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230504082721.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s2006 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11340-006-9112-7</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2058173465</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s11340-006-9112-7-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">690</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Yang, H.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Improvement of Fourier Polarimetry for Applications in Tomographic Photoelasticity</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2006</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Society for Experimental Mechanics 2006</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The use of the Fourier Polarimetry method has been demonstrated to extract the three characteristic parameters in integrated photoelasticity. In contrast to the phase-stepping method, it has been shown that the Fourier method is more accurate. However, the Fourier method isn't very efficient as it requires that a minimum of nine intensity images be collected during a whole revolution of a polarizer while the phase-stepping method only needs six intensity images. In this paper the Fourier transformation is used to derive the expression for determination of the characteristic parameters. Four Fourier coefficients are clearly identified to calculate the three characteristic parameters. It is found that the angular rotation ratio could be set arbitrarily. The angular rotation ratio is optimized to satisfy the requirements of efficiency and proper data accuracy, which results in data collection about three times faster than the methods suggested by previous researchers. When comparing their performance in terms of efficiency and accuracy, the simulated and experimental results show that these angular rotation ratios have the same accuracy but the optimized angular rotation ratio is significantly faster. The sensitivity to noise is also investigated and further improvement of accuracy is suggested.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Three-dimensional photoelasticity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Fourier Polarimetry</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Tomographic photoelasticity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Integrated photoelasticity</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gibson, S.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tomlinson, R. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Experimental mechanics</subfield><subfield code="d">Kluwer Academic Publishers, 1961</subfield><subfield code="g">46(2006), 5 vom: 25. Juli, Seite 619-626</subfield><subfield code="w">(DE-627)129593990</subfield><subfield code="w">(DE-600)240480-1</subfield><subfield code="w">(DE-576)015086852</subfield><subfield code="x">0014-4851</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:46</subfield><subfield code="g">year:2006</subfield><subfield code="g">number:5</subfield><subfield code="g">day:25</subfield><subfield code="g">month:07</subfield><subfield code="g">pages:619-626</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s11340-006-9112-7</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-UMW</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-ARC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2057</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4317</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">46</subfield><subfield code="j">2006</subfield><subfield code="e">5</subfield><subfield code="b">25</subfield><subfield code="c">07</subfield><subfield code="h">619-626</subfield></datafield></record></collection>
|
score |
7.401023 |