{"refrec":{"BRefID":353558,"RR":"<b>Hubert, M.; Trosman, O.; Collard, Y.; Sukhov, A.; Harting, J.; Vandewalle, N.; Smith, A.-S.</b> (2021). Scallop theorem and swimming at the mesoscale. <i>Phys. Rev. Lett. 126(22)</i>: 224501. <a href=\"https://dx.doi.org/10.1103/PhysRevLett.126.224501\" target=\"_blank\">https://dx.doi.org/10.1103/PhysRevLett.126.224501</a>","BEntID":351268,"PublicFlag":1,"CheckedFlag":1,"wosflag":1,"vabbflag":1,"RefStringPartII":". <i>Phys. Rev. Lett. 126(22)</i>: 224501. <a href=\"https://dx.doi.org/10.1103/PhysRevLett.126.224501\" target=\"_blank\">https://dx.doi.org/10.1103/PhysRevLett.126.224501</a>","DocTypID":8,"DocType":"Journal article","MarineFlag":1,"FreshFlag":0,"BrackishFlag":0,"TerrestrialFlag":0,"Authorstring":"Hubert, M.; Trosman, O.; Collard, Y.; Sukhov, A.; Harting, J.; Vandewalle, N.; Smith, A.-S.","OrigTitleTranslFlag":0,"Authorstringtrunc":"Hubert, M. <i>et al.</i>","Englishabstract":"By comparing theoretical modeling, simulations, and experiments, we show that there exists a swimming regime at low Reynolds numbers solely driven by the inertia of the swimmer itself. This is demonstrated by considering a dumbbell with an asymmetry in coasting time in its two spheres. Despite deforming in a reciprocal fashion, the dumbbell swims by generating a nonreciprocal Stokesian flow, which arises from the asymmetry in coasting times. 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