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Direct observation of dynamic shear jamming in dense suspensions

Direct observation of dynamic shear jamming in dense suspensions
Direct observation of dynamic shear jamming in dense suspensions
Liquid-like at rest, dense suspensions of hard particles can undergo striking transformations in behaviour when agitated or sheared1. These phenomena include solidification during rapid impact2,3, as well as strong shear thickening characterized by discontinuous, orders of magnitude increases in suspension viscosity4-8. Much of this highly non-Newtonian behaviour has recently been interpreted within the framework of a jamming transition. However, while jamming indeed induces solid-like rigidity9-11, even a strongly shear-thickened state still flows and thus cannot be fully jammed12,13. Furthermore, while suspensions are incompressible, the onset of rigidity in the standard jamming scenario requires an increase in particle density9,10,14. Finally, while shear thickening occurs in the steady state, impact-induced solidification is transient15-17. As a result, it has remained unsettled how these dense suspension phenomena are related and how they are connected to jamming. Here we resolve this by systematically exploring both the steady-state and transient regimes with the same experimental system. We demonstrate that a fully jammed, solid-like state can be reached without compression and instead purely by shear, as recently proposed for dry granular systems18,19. In contrast to dry granular materials, however, this state is created by transient shear-jamming fronts, which we track for the first time directly. We also show that shear stress, rather than shear rate, is the key control parameter. From these findings we map out a state diagram with particle density and shear stress as variables. Discontinuous shear thickening is newly identified with a marginally jammed regime just below the onset of full, solid-like jamming20. This state diagram provides a new, unifying framework, compatible with prior experimental and simulation results on dense suspensions, that connects steady-state and transient behaviour in terms of a dynamic shear-jamming process.
0028-0836
214-217
Peters, I.
222d846e-e620-4017-84cb-099b14ff2d75
Majumdar, S.
cb1939da-8feb-47f1-9e7f-23e3e72c651d
Jaeger, H.M.
7b2b1669-0182-417f-9ec3-63d5f7806528
Peters, I.
222d846e-e620-4017-84cb-099b14ff2d75
Majumdar, S.
cb1939da-8feb-47f1-9e7f-23e3e72c651d
Jaeger, H.M.
7b2b1669-0182-417f-9ec3-63d5f7806528

Peters, I., Majumdar, S. and Jaeger, H.M. (2016) Direct observation of dynamic shear jamming in dense suspensions. Nature, 532, 214-217. (doi:10.1038/nature17167).

Record type: Article

Abstract

Liquid-like at rest, dense suspensions of hard particles can undergo striking transformations in behaviour when agitated or sheared1. These phenomena include solidification during rapid impact2,3, as well as strong shear thickening characterized by discontinuous, orders of magnitude increases in suspension viscosity4-8. Much of this highly non-Newtonian behaviour has recently been interpreted within the framework of a jamming transition. However, while jamming indeed induces solid-like rigidity9-11, even a strongly shear-thickened state still flows and thus cannot be fully jammed12,13. Furthermore, while suspensions are incompressible, the onset of rigidity in the standard jamming scenario requires an increase in particle density9,10,14. Finally, while shear thickening occurs in the steady state, impact-induced solidification is transient15-17. As a result, it has remained unsettled how these dense suspension phenomena are related and how they are connected to jamming. Here we resolve this by systematically exploring both the steady-state and transient regimes with the same experimental system. We demonstrate that a fully jammed, solid-like state can be reached without compression and instead purely by shear, as recently proposed for dry granular systems18,19. In contrast to dry granular materials, however, this state is created by transient shear-jamming fronts, which we track for the first time directly. We also show that shear stress, rather than shear rate, is the key control parameter. From these findings we map out a state diagram with particle density and shear stress as variables. Discontinuous shear thickening is newly identified with a marginally jammed regime just below the onset of full, solid-like jamming20. This state diagram provides a new, unifying framework, compatible with prior experimental and simulation results on dense suspensions, that connects steady-state and transient behaviour in terms of a dynamic shear-jamming process.

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Accepted/In Press date: 20 January 2016
e-pub ahead of print date: 4 April 2016
Published date: 14 April 2016
Organisations: Aerodynamics & Flight Mechanics Group

Identifiers

Local EPrints ID: 388218
URI: http://eprints.soton.ac.uk/id/eprint/388218
ISSN: 0028-0836
PURE UUID: 8c8ca255-e59f-425c-bdb3-f1025d0b45e8
ORCID for I. Peters: ORCID iD orcid.org/0000-0002-3549-3322

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Date deposited: 22 Feb 2016 11:59
Last modified: 15 Mar 2024 03:52

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Contributors

Author: I. Peters ORCID iD
Author: S. Majumdar
Author: H.M. Jaeger

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