|
|
|
|
LEADER |
01831nam a2200325Ia 4500 |
001 |
10.1063-5.0085773 |
008 |
220510s2022 CNT 000 0 und d |
020 |
|
|
|a 00219606 (ISSN)
|
245 |
1 |
0 |
|a Delayed elastic contributions to the viscoelastic response of foams
|
260 |
|
0 |
|b American Institute of Physics Inc.
|c 2022
|
856 |
|
|
|z View Fulltext in Publisher
|u https://doi.org/10.1063/5.0085773
|
520 |
3 |
|
|a We show that the slow viscoelastic response of a foam is that of a power-law fluid with a terminal relaxation. Investigations of the foam mechanics in creep and recovery tests reveal that the power-law contribution is fully reversible, indicative of a delayed elastic response. We demonstrate how this contribution fully accounts for the non-Maxwellian features observed in all tests, probing the linear mechanical response function. The associated power-law spectrum is consistent with soft glassy rheology of systems with mechanical noise temperatures just above the glass transition [Fielding et al., J. Rheol. 44, 323 (2000)] and originates from a combination of superdiffusive bubble dynamics and stress diffusion, as recently evidenced in simulations of coarsening foam [Hwang et al., Nat. Mater. 15, 1031 (2016)]. © 2022 Author(s).
|
650 |
0 |
4 |
|a A: Foams
|
650 |
0 |
4 |
|a Coarsening
|
650 |
0 |
4 |
|a Creep and recovery tests
|
650 |
0 |
4 |
|a Elastic contribution
|
650 |
0 |
4 |
|a Elastic response
|
650 |
0 |
4 |
|a Foam mechanics
|
650 |
0 |
4 |
|a Glass
|
650 |
0 |
4 |
|a Glass transition
|
650 |
0 |
4 |
|a Mechanical response
|
650 |
0 |
4 |
|a Power law fluid
|
650 |
0 |
4 |
|a Power-law contribution
|
650 |
0 |
4 |
|a Response functions
|
650 |
0 |
4 |
|a Viscoelastic response
|
650 |
0 |
4 |
|a Viscoelasticity
|
700 |
1 |
|
|a Lavergne, F.A.
|e author
|
700 |
1 |
|
|a Sollich, P.
|e author
|
700 |
1 |
|
|a Trappe, V.
|e author
|
773 |
|
|
|t Journal of Chemical Physics
|