A direct relation between bending energy and contact angles for capillary bridges
The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free su...
Ausführliche Beschreibung
Autor*in: |
Millet, Olivier [verfasserIn] Gagneux , Gérard [verfasserIn] |
---|
Format: |
E-Artikel |
---|---|
Sprache: |
Englisch ; Französisch |
Erschienen: |
2023 |
---|
Schlagwörter: |
Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Generalized Young–Laplace equation |
---|
Übergeordnetes Werk: |
In: Comptes Rendus. Mécanique - Académie des sciences, 2022, 351(2023), S2, Seite 125-137 |
---|---|
Übergeordnetes Werk: |
volume:351 ; year:2023 ; number:S2 ; pages:125-137 |
Links: |
---|
DOI / URN: |
10.5802/crmeca.200 |
---|
Katalog-ID: |
DOAJ092554946 |
---|
LEADER | 01000caa a22002652 4500 | ||
---|---|---|---|
001 | DOAJ092554946 | ||
003 | DE-627 | ||
005 | 20240414124436.0 | ||
007 | cr uuu---uuuuu | ||
008 | 240412s2023 xx |||||o 00| ||eng c | ||
024 | 7 | |a 10.5802/crmeca.200 |2 doi | |
035 | |a (DE-627)DOAJ092554946 | ||
035 | |a (DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451 | ||
040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
041 | |a eng |a fre | ||
050 | 0 | |a TA401-492 | |
100 | 0 | |a Millet, Olivier |e verfasserin |4 aut | |
245 | 1 | 2 | |a A direct relation between bending energy and contact angles for capillary bridges |
264 | 1 | |c 2023 | |
336 | |a Text |b txt |2 rdacontent | ||
337 | |a Computermedien |b c |2 rdamedia | ||
338 | |a Online-Ressource |b cr |2 rdacarrier | ||
520 | |a The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. | ||
650 | 4 | |a Distortion of nonaxisymmetric capillary bridges | |
650 | 4 | |a Mean and Gaussian curvatures impact | |
650 | 4 | |a Euler characteristic | |
650 | 4 | |a Generalized Young–Laplace equation | |
650 | 4 | |a Bending effects | |
650 | 4 | |a Fenchel’s theorem in differential geometry | |
650 | 4 | |a Gauss–Bonnet Theorem | |
650 | 4 | |a Geodesic curvature | |
650 | 4 | |a Bending stress | |
650 | 4 | |a Influence of the contact angles | |
653 | 0 | |a Materials of engineering and construction. Mechanics of materials | |
700 | 0 | |a Gagneux , Gérard |e verfasserin |4 aut | |
773 | 0 | 8 | |i In |t Comptes Rendus. Mécanique |d Académie des sciences, 2022 |g 351(2023), S2, Seite 125-137 |w (DE-627)348585381 |w (DE-600)2079504-X |x 18737234 |7 nnns |
773 | 1 | 8 | |g volume:351 |g year:2023 |g number:S2 |g pages:125-137 |
856 | 4 | 0 | |u https://doi.org/10.5802/crmeca.200 |z kostenfrei |
856 | 4 | 0 | |u https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451 |z kostenfrei |
856 | 4 | 0 | |u https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/ |z kostenfrei |
856 | 4 | 2 | |u https://doaj.org/toc/1873-7234 |y Journal toc |z kostenfrei |
912 | |a GBV_USEFLAG_A | ||
912 | |a SYSFLAG_A | ||
912 | |a GBV_DOAJ | ||
912 | |a GBV_ILN_11 | ||
912 | |a GBV_ILN_20 | ||
912 | |a GBV_ILN_22 | ||
912 | |a GBV_ILN_23 | ||
912 | |a GBV_ILN_24 | ||
912 | |a GBV_ILN_31 | ||
912 | |a GBV_ILN_39 | ||
912 | |a GBV_ILN_40 | ||
912 | |a GBV_ILN_60 | ||
912 | |a GBV_ILN_62 | ||
912 | |a GBV_ILN_63 | ||
912 | |a GBV_ILN_65 | ||
912 | |a GBV_ILN_69 | ||
912 | |a GBV_ILN_70 | ||
912 | |a GBV_ILN_73 | ||
912 | |a GBV_ILN_95 | ||
912 | |a GBV_ILN_105 | ||
912 | |a GBV_ILN_110 | ||
912 | |a GBV_ILN_151 | ||
912 | |a GBV_ILN_161 | ||
912 | |a GBV_ILN_165 | ||
912 | |a GBV_ILN_170 | ||
912 | |a GBV_ILN_213 | ||
912 | |a GBV_ILN_230 | ||
912 | |a GBV_ILN_285 | ||
912 | |a GBV_ILN_293 | ||
912 | |a GBV_ILN_370 | ||
912 | |a GBV_ILN_602 | ||
912 | |a GBV_ILN_2004 | ||
912 | |a GBV_ILN_2014 | ||
912 | |a GBV_ILN_2336 | ||
912 | |a GBV_ILN_4012 | ||
912 | |a GBV_ILN_4037 | ||
912 | |a GBV_ILN_4112 | ||
912 | |a GBV_ILN_4125 | ||
912 | |a GBV_ILN_4126 | ||
912 | |a GBV_ILN_4249 | ||
912 | |a GBV_ILN_4305 | ||
912 | |a GBV_ILN_4306 | ||
912 | |a GBV_ILN_4307 | ||
912 | |a GBV_ILN_4313 | ||
912 | |a GBV_ILN_4322 | ||
912 | |a GBV_ILN_4323 | ||
912 | |a GBV_ILN_4324 | ||
912 | |a GBV_ILN_4325 | ||
912 | |a GBV_ILN_4335 | ||
912 | |a GBV_ILN_4338 | ||
912 | |a GBV_ILN_4367 | ||
912 | |a GBV_ILN_4700 | ||
951 | |a AR | ||
952 | |d 351 |j 2023 |e S2 |h 125-137 |
author_variant |
o m om g g g gg |
---|---|
matchkey_str |
article:18737234:2023----::drcrltobtenedneegadotcage |
hierarchy_sort_str |
2023 |
callnumber-subject-code |
TA |
publishDate |
2023 |
allfields |
10.5802/crmeca.200 doi (DE-627)DOAJ092554946 (DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451 DE-627 ger DE-627 rakwb eng fre TA401-492 Millet, Olivier verfasserin aut A direct relation between bending energy and contact angles for capillary bridges 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Euler characteristic Generalized Young–Laplace equation Bending effects Fenchel’s theorem in differential geometry Gauss–Bonnet Theorem Geodesic curvature Bending stress Influence of the contact angles Materials of engineering and construction. Mechanics of materials Gagneux , Gérard verfasserin aut In Comptes Rendus. Mécanique Académie des sciences, 2022 351(2023), S2, Seite 125-137 (DE-627)348585381 (DE-600)2079504-X 18737234 nnns volume:351 year:2023 number:S2 pages:125-137 https://doi.org/10.5802/crmeca.200 kostenfrei https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451 kostenfrei https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/ kostenfrei https://doaj.org/toc/1873-7234 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_165 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 351 2023 S2 125-137 |
spelling |
10.5802/crmeca.200 doi (DE-627)DOAJ092554946 (DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451 DE-627 ger DE-627 rakwb eng fre TA401-492 Millet, Olivier verfasserin aut A direct relation between bending energy and contact angles for capillary bridges 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Euler characteristic Generalized Young–Laplace equation Bending effects Fenchel’s theorem in differential geometry Gauss–Bonnet Theorem Geodesic curvature Bending stress Influence of the contact angles Materials of engineering and construction. Mechanics of materials Gagneux , Gérard verfasserin aut In Comptes Rendus. Mécanique Académie des sciences, 2022 351(2023), S2, Seite 125-137 (DE-627)348585381 (DE-600)2079504-X 18737234 nnns volume:351 year:2023 number:S2 pages:125-137 https://doi.org/10.5802/crmeca.200 kostenfrei https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451 kostenfrei https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/ kostenfrei https://doaj.org/toc/1873-7234 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_165 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 351 2023 S2 125-137 |
allfields_unstemmed |
10.5802/crmeca.200 doi (DE-627)DOAJ092554946 (DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451 DE-627 ger DE-627 rakwb eng fre TA401-492 Millet, Olivier verfasserin aut A direct relation between bending energy and contact angles for capillary bridges 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Euler characteristic Generalized Young–Laplace equation Bending effects Fenchel’s theorem in differential geometry Gauss–Bonnet Theorem Geodesic curvature Bending stress Influence of the contact angles Materials of engineering and construction. Mechanics of materials Gagneux , Gérard verfasserin aut In Comptes Rendus. Mécanique Académie des sciences, 2022 351(2023), S2, Seite 125-137 (DE-627)348585381 (DE-600)2079504-X 18737234 nnns volume:351 year:2023 number:S2 pages:125-137 https://doi.org/10.5802/crmeca.200 kostenfrei https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451 kostenfrei https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/ kostenfrei https://doaj.org/toc/1873-7234 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_165 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 351 2023 S2 125-137 |
allfieldsGer |
10.5802/crmeca.200 doi (DE-627)DOAJ092554946 (DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451 DE-627 ger DE-627 rakwb eng fre TA401-492 Millet, Olivier verfasserin aut A direct relation between bending energy and contact angles for capillary bridges 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Euler characteristic Generalized Young–Laplace equation Bending effects Fenchel’s theorem in differential geometry Gauss–Bonnet Theorem Geodesic curvature Bending stress Influence of the contact angles Materials of engineering and construction. Mechanics of materials Gagneux , Gérard verfasserin aut In Comptes Rendus. Mécanique Académie des sciences, 2022 351(2023), S2, Seite 125-137 (DE-627)348585381 (DE-600)2079504-X 18737234 nnns volume:351 year:2023 number:S2 pages:125-137 https://doi.org/10.5802/crmeca.200 kostenfrei https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451 kostenfrei https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/ kostenfrei https://doaj.org/toc/1873-7234 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_165 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 351 2023 S2 125-137 |
allfieldsSound |
10.5802/crmeca.200 doi (DE-627)DOAJ092554946 (DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451 DE-627 ger DE-627 rakwb eng fre TA401-492 Millet, Olivier verfasserin aut A direct relation between bending energy and contact angles for capillary bridges 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Euler characteristic Generalized Young–Laplace equation Bending effects Fenchel’s theorem in differential geometry Gauss–Bonnet Theorem Geodesic curvature Bending stress Influence of the contact angles Materials of engineering and construction. Mechanics of materials Gagneux , Gérard verfasserin aut In Comptes Rendus. Mécanique Académie des sciences, 2022 351(2023), S2, Seite 125-137 (DE-627)348585381 (DE-600)2079504-X 18737234 nnns volume:351 year:2023 number:S2 pages:125-137 https://doi.org/10.5802/crmeca.200 kostenfrei https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451 kostenfrei https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/ kostenfrei https://doaj.org/toc/1873-7234 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_165 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 351 2023 S2 125-137 |
language |
English French |
source |
In Comptes Rendus. Mécanique 351(2023), S2, Seite 125-137 volume:351 year:2023 number:S2 pages:125-137 |
sourceStr |
In Comptes Rendus. Mécanique 351(2023), S2, Seite 125-137 volume:351 year:2023 number:S2 pages:125-137 |
format_phy_str_mv |
Article |
institution |
findex.gbv.de |
topic_facet |
Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Euler characteristic Generalized Young–Laplace equation Bending effects Fenchel’s theorem in differential geometry Gauss–Bonnet Theorem Geodesic curvature Bending stress Influence of the contact angles Materials of engineering and construction. Mechanics of materials |
isfreeaccess_bool |
true |
container_title |
Comptes Rendus. Mécanique |
authorswithroles_txt_mv |
Millet, Olivier @@aut@@ Gagneux , Gérard @@aut@@ |
publishDateDaySort_date |
2023-01-01T00:00:00Z |
hierarchy_top_id |
348585381 |
id |
DOAJ092554946 |
language_de |
englisch franzoesisch |
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">DOAJ092554946</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20240414124436.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">240412s2023 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.5802/crmeca.200</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ092554946</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451</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><subfield code="a">fre</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">TA401-492</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Millet, Olivier</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="2"><subfield code="a">A direct relation between bending energy and contact angles for capillary bridges</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2023</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">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Distortion of nonaxisymmetric capillary bridges</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Mean and Gaussian curvatures impact</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Euler characteristic</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Generalized Young–Laplace equation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Bending effects</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Fenchel’s theorem in differential geometry</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Gauss–Bonnet Theorem</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Geodesic curvature</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Bending stress</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Influence of the contact angles</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Materials of engineering and construction. Mechanics of materials</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Gagneux , Gérard</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">Comptes Rendus. Mécanique</subfield><subfield code="d">Académie des sciences, 2022</subfield><subfield code="g">351(2023), S2, Seite 125-137</subfield><subfield code="w">(DE-627)348585381</subfield><subfield code="w">(DE-600)2079504-X</subfield><subfield code="x">18737234</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:351</subfield><subfield code="g">year:2023</subfield><subfield code="g">number:S2</subfield><subfield code="g">pages:125-137</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.5802/crmeca.200</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/1873-7234</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</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_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</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_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</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_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</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_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_165</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</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">351</subfield><subfield code="j">2023</subfield><subfield code="e">S2</subfield><subfield code="h">125-137</subfield></datafield></record></collection>
|
callnumber-first |
T - Technology |
author |
Millet, Olivier |
spellingShingle |
Millet, Olivier misc TA401-492 misc Distortion of nonaxisymmetric capillary bridges misc Mean and Gaussian curvatures impact misc Euler characteristic misc Generalized Young–Laplace equation misc Bending effects misc Fenchel’s theorem in differential geometry misc Gauss–Bonnet Theorem misc Geodesic curvature misc Bending stress misc Influence of the contact angles misc Materials of engineering and construction. Mechanics of materials A direct relation between bending energy and contact angles for capillary bridges |
authorStr |
Millet, Olivier |
ppnlink_with_tag_str_mv |
@@773@@(DE-627)348585381 |
format |
electronic Article |
delete_txt_mv |
keep |
author_role |
aut aut |
collection |
DOAJ |
remote_str |
true |
callnumber-label |
TA401-492 |
illustrated |
Not Illustrated |
issn |
18737234 |
topic_title |
TA401-492 A direct relation between bending energy and contact angles for capillary bridges Distortion of nonaxisymmetric capillary bridges Mean and Gaussian curvatures impact Euler characteristic Generalized Young–Laplace equation Bending effects Fenchel’s theorem in differential geometry Gauss–Bonnet Theorem Geodesic curvature Bending stress Influence of the contact angles |
topic |
misc TA401-492 misc Distortion of nonaxisymmetric capillary bridges misc Mean and Gaussian curvatures impact misc Euler characteristic misc Generalized Young–Laplace equation misc Bending effects misc Fenchel’s theorem in differential geometry misc Gauss–Bonnet Theorem misc Geodesic curvature misc Bending stress misc Influence of the contact angles misc Materials of engineering and construction. Mechanics of materials |
topic_unstemmed |
misc TA401-492 misc Distortion of nonaxisymmetric capillary bridges misc Mean and Gaussian curvatures impact misc Euler characteristic misc Generalized Young–Laplace equation misc Bending effects misc Fenchel’s theorem in differential geometry misc Gauss–Bonnet Theorem misc Geodesic curvature misc Bending stress misc Influence of the contact angles misc Materials of engineering and construction. Mechanics of materials |
topic_browse |
misc TA401-492 misc Distortion of nonaxisymmetric capillary bridges misc Mean and Gaussian curvatures impact misc Euler characteristic misc Generalized Young–Laplace equation misc Bending effects misc Fenchel’s theorem in differential geometry misc Gauss–Bonnet Theorem misc Geodesic curvature misc Bending stress misc Influence of the contact angles misc Materials of engineering and construction. Mechanics of materials |
format_facet |
Elektronische Aufsätze Aufsätze Elektronische Ressource |
format_main_str_mv |
Text Zeitschrift/Artikel |
carriertype_str_mv |
cr |
hierarchy_parent_title |
Comptes Rendus. Mécanique |
hierarchy_parent_id |
348585381 |
hierarchy_top_title |
Comptes Rendus. Mécanique |
isfreeaccess_txt |
true |
familylinks_str_mv |
(DE-627)348585381 (DE-600)2079504-X |
title |
A direct relation between bending energy and contact angles for capillary bridges |
ctrlnum |
(DE-627)DOAJ092554946 (DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451 |
title_full |
A direct relation between bending energy and contact angles for capillary bridges |
author_sort |
Millet, Olivier |
journal |
Comptes Rendus. Mécanique |
journalStr |
Comptes Rendus. Mécanique |
callnumber-first-code |
T |
lang_code |
eng fre |
isOA_bool |
true |
recordtype |
marc |
publishDateSort |
2023 |
contenttype_str_mv |
txt |
container_start_page |
125 |
author_browse |
Millet, Olivier Gagneux , Gérard |
container_volume |
351 |
class |
TA401-492 |
format_se |
Elektronische Aufsätze |
author-letter |
Millet, Olivier |
doi_str_mv |
10.5802/crmeca.200 |
author2-role |
verfasserin |
title_sort |
direct relation between bending energy and contact angles for capillary bridges |
callnumber |
TA401-492 |
title_auth |
A direct relation between bending energy and contact angles for capillary bridges |
abstract |
The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. |
abstractGer |
The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. |
abstract_unstemmed |
The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line. |
collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_165 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 |
container_issue |
S2 |
title_short |
A direct relation between bending energy and contact angles for capillary bridges |
url |
https://doi.org/10.5802/crmeca.200 https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451 https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/ https://doaj.org/toc/1873-7234 |
remote_bool |
true |
author2 |
Gagneux , Gérard |
author2Str |
Gagneux , Gérard |
ppnlink |
348585381 |
callnumber-subject |
TA - General and Civil Engineering |
mediatype_str_mv |
c |
isOA_txt |
true |
hochschulschrift_bool |
false |
doi_str |
10.5802/crmeca.200 |
callnumber-a |
TA401-492 |
up_date |
2024-07-04T01:44:35.413Z |
_version_ |
1803610987339710464 |
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">DOAJ092554946</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20240414124436.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">240412s2023 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.5802/crmeca.200</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ092554946</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ4d7b1ecc5b25474ea8baac851ae66451</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><subfield code="a">fre</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">TA401-492</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Millet, Olivier</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="2"><subfield code="a">A direct relation between bending energy and contact angles for capillary bridges</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2023</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">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The didactic object of these developments on differential geometry of curves and surfaces is to present fine and convenient mathematical strategies, adapted to the study of capillary bridges. The common thread is to be able to calculate accurately in any situation the bending stress over the free surface, represented mathematically by the integral of the Gaussian curvature over the surface (called the total curvature) involved in the generalized Young–Laplace equation. We prove in particular that the resultant of the bending energy is directly linked to the wetting angles at the contact line.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Distortion of nonaxisymmetric capillary bridges</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Mean and Gaussian curvatures impact</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Euler characteristic</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Generalized Young–Laplace equation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Bending effects</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Fenchel’s theorem in differential geometry</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Gauss–Bonnet Theorem</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Geodesic curvature</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Bending stress</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Influence of the contact angles</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Materials of engineering and construction. Mechanics of materials</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Gagneux , Gérard</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">Comptes Rendus. Mécanique</subfield><subfield code="d">Académie des sciences, 2022</subfield><subfield code="g">351(2023), S2, Seite 125-137</subfield><subfield code="w">(DE-627)348585381</subfield><subfield code="w">(DE-600)2079504-X</subfield><subfield code="x">18737234</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:351</subfield><subfield code="g">year:2023</subfield><subfield code="g">number:S2</subfield><subfield code="g">pages:125-137</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.5802/crmeca.200</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/4d7b1ecc5b25474ea8baac851ae66451</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://comptes-rendus.academie-sciences.fr/mecanique/articles/10.5802/crmeca.200/</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/1873-7234</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</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_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</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_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</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_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</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_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_165</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2336</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</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">351</subfield><subfield code="j">2023</subfield><subfield code="e">S2</subfield><subfield code="h">125-137</subfield></datafield></record></collection>
|
score |
7.400462 |