000820713 001__ 820713 000820713 005__ 20240610115401.0 000820713 0247_ $$2doi$$a10.1140/epjst/e2016-60070-6 000820713 0247_ $$2ISSN$$a1951-6355 000820713 0247_ $$2ISSN$$a1951-6401 000820713 0247_ $$2Handle$$a2128/12748 000820713 0247_ $$2WOS$$aWOS:000387062100018 000820713 037__ $$aFZJ-2016-05981 000820713 082__ $$a530 000820713 1001_ $$0P:(DE-Juel1)130629$$aElgeti, Jens$$b0$$eCorresponding author 000820713 245__ $$aMicroswimmers near surfaces 000820713 260__ $$aBerlin$$bSpringer$$c2016 000820713 3367_ $$2DRIVER$$aarticle 000820713 3367_ $$2DataCite$$aOutput Types/Journal article 000820713 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1478845436_32296 000820713 3367_ $$2BibTeX$$aARTICLE 000820713 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000820713 3367_ $$00$$2EndNote$$aJournal Article 000820713 520__ $$aBoth, in their natural environment and in a controlled experimental setup, microswimmers regularly interact with surfaces. These surfaces provide a steric boundary, both for the swimming motion and the hydrodynamic flow pattern. These effects typically imply a strong accumulation of microswimmers near surfaces. While some generic features can be derived, details of the swimmer shape and propulsion mechanism matter, which give rise to a broad range of adhesion phenomena and have to be taken into account to predict the surface accumulation for a given swimmer. 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