Open Access Article
Noémie
Dagès
a,
Louis V.
Bouthier
b,
Lauren
Matthews
c,
Sébastien
Manneville
a,
Thibaut
Divoux
a,
Arnaud
Poulesquen
d and
Thomas
Gibaud
*a
aUniv Lyon, Ens de Lyon, Univ Claude Bernard, CNRS, Laboratoire de Physique, F69342 Lyon, France. E-mail: thomas.gibaud@ens-lyon.fr
bGroupe CFL, CEMEF, Mines Paristech, 1 Rue Claude Daunesse, 06904 Sophia Antipolis, France
cESRF – The European Synchrotron, 38043 Grenoble Cedex, France
dCEA, DES, ISEC, DE2D, SEAD, LCBC, Université of Montpellier, Marcoule, France
First published on 7th October 2022
Correction for ‘Interpenetration of fractal clusters drives elasticity in colloidal gels formed upon flow cessation’ by Noémie Dagès et al., Soft Matter, 2022, 18, 6645–6659, https://doi.org/10.1039/D2SM00481J.
in eqn (1) and (15). The corrected calculation of
corroborates the experimental data presented in Fig. 4c of the published article. The paper’s conclusion remains therefore unchanged.
In the published article, in eqn (8), the conservation of mass is expressed as
![]() | (1) |
![]() | (2) |
![]() | (3) |
![]() | (4) |
Fig. 4c in the published article displays the variations of the gel crossover elasticity Gc as a function of the shear rate intensity
0 applied before flow cessation and the fit using the interpenetration ϕ-power law model. We note that
. The fit of Gc in this figure needs to be modified accordingly to eqn (4) above and replaced by Fig. 1 shown here. In this Fig. 1, the corrected model fits well the data. The conclusion of the paper remains therefore unchanged.
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Fig. 1 Evolution of Gcvs. 0. The red line is the best fit of the data using eqn (4) here and the structural information reported in Fig. 6a of the published article. The best fit is obtained with a single adjustable parameter, namely the prefactor GCB = 9 Pa. | ||
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