title: Dynamics of Rear Stagnant Cap formation at the surface of spherical bubbles rising in surfactant solutions at large Reynolds numbers under conditions of small Marangoni number and slow sorption kinetics.
abstract: On the surface of bubbles rising in a surfactant solution the adsorption process proceeds and leads to the formation of a so called Rear Stagnant Cap (RSC). The larger this RSC is the stronger is the retardation of the rising velocity. The theory of a steady RSC and steady retarded rising velocity, which sets in after a transient stage, has been generally accepted. However, a non-steady process of bubble rising starting from the initial zero velocity represents an important portion of the trajectory of rising, characterized by a local velocity profile (LVP). As there is no theory of RSC growth for large Reynolds numbers Re » 1 so far, the interpretation of LVPs measured in this regime was impossible. It turned out, that an analytical theory for a quasi-steady growth of RSC is possible for small Marangoni numbers Ma « 1, i.e. when the RSC is almost completely compressed, which means a uniform surface concentration Γ(θ)=Γ(∞) within the RSC. Hence, the RSC angle ψ(t) is obtained as a function of the adsorption isotherm parameters and time t. From the steady velocity v(st)(ψ), the dependence of non-steady velocity on time is obtained by employing v(st)[ψ(t)] via a quasi-steady approximation. The measurement of LVP creates a promising new opportunity for investigation of the RSC dynamics and adsorption kinetics. While adsorption and desorption happen at the same localization in the classical methods, in rising bubble experiments desorption occurs mainly within RSC while adsorption on the mobile part of the bubble surface. The desorption flux from RSC is proportional to αΓ(∞), while it is usually αΓ. The adsorption flux at the mobile surface above RSC can be assumed proportional to βC0, while it is usually βC0(1-Γ/Γ(∞)). These simplifications may become favorable in investigations of the adsorption kinetics for larger molecules, in particular for globular proteins, which essentially stay at an interface once adsorbed.
authors.affiliation: Department of Civil and Environment Engineering, New Jersey Institute of Technology, University Heights, Newark, NJ 07102, USA.
authors.forename: S S
authors.initials: SS
authors.lastname: Dukhin
authors.affiliation: Institute of Biocolloid Chemistry, 42 Vernadsky Avenue, 03680 Kiev, Ukraine.
authors.forename: V I
authors.initials: VI
authors.lastname: Kovalchuk
authors.affiliation: Max-Planck-Institut für Kolloid- und Grenzflächenforschung, 14424 Potsdam, Germany; Institute of Physical Chemistry, Bulgarian Academy of Sciences, 1113 Sofia, Bulgaria. Electronic address: georgi.gochev@mpikg.mpg.de.
authors.forename: G G
authors.initials: GG
authors.lastname: Gochev
authors.affiliation: Max-Planck-Institut für Kolloid- und Grenzflächenforschung, 14424 Potsdam, Germany; Sharif University of Technology, Tehran, Iran.
authors.forename: M
authors.initials: M
authors.lastname: Lotfi
authors.affiliation: Jerzy Haber Institute of Catalysis and Surface Chemistry Polish Academy of Sciences, Niezapominajek 8, 30-239 Cracow, Poland.
authors.forename: M
authors.initials: M
authors.lastname: Krzan
authors.affiliation: Jerzy Haber Institute of Catalysis and Surface Chemistry Polish Academy of Sciences, Niezapominajek 8, 30-239 Cracow, Poland.
authors.forename: K
authors.initials: K
authors.lastname: Malysa
authors.affiliation: Max-Planck-Institut für Kolloid- und Grenzflächenforschung, 14424 Potsdam, Germany.
authors.forename: R
authors.initials: R
authors.lastname: Miller
keywords: Bubble rising retardation; Large Reynolds number (Re); Local velocity profile (LVP); Rear stagnant cap (RSC); Small Marangoni number (Ma); Surfactant and protein adsorption kinetics