2016
DOI: 10.1155/2016/1716598
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Normal Stress Differences and Yield Stresses in Attractive Particle Networks

Abstract: The nature of attractive particulate networks, yield stresses, and normal stress differences is systematically reviewed, each in terms of the relevant definitions, underlying mechanisms, and current measurement techniques. With this foundation, experimental observations of normal stress differences in some suspensions and colloidal systems are surveyed, along with constitutive models that allow for normal stress differences to arise prior to yielding. Yield stresses are a hallmark of attractive colloidal syste… Show more

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Cited by 13 publications
(6 citation statements)
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References 129 publications
(263 reference statements)
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“…1D and E , respectively). Normal force is characterised as a normal stress difference (Δ N = N 1 − N 2 ), where N 1 and N 2 are the primary and secondary normal stress differences, respectively (see definition in ‘Materials and methods’ 28 ). The fluid’s elasticity dominates the viscous flow properties for the wild-type biofilm matrix extracted by EMIM-Ac, whereby Δ N is an order of magnitude greater than shear stress (Fig.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…1D and E , respectively). Normal force is characterised as a normal stress difference (Δ N = N 1 − N 2 ), where N 1 and N 2 are the primary and secondary normal stress differences, respectively (see definition in ‘Materials and methods’ 28 ). The fluid’s elasticity dominates the viscous flow properties for the wild-type biofilm matrix extracted by EMIM-Ac, whereby Δ N is an order of magnitude greater than shear stress (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Forty milligrams per millilitre solutions of lyophilised biofilms were added to 1 mL EMIM-Ac and incubated at 55 °C for 2 h. A Haake Mars 3 (Thermo Fisher Scientific) stress-controlled rotational rheometer with Peltier-controlled element at 25 °C was used for rheological measurements. Thirty-five-millimetre-diameter parallel plate geometry was used with smooth titanium plates to measure viscosity and normal stress difference ( N 1 − N 2 ), where N 1 is the difference between normal stresses in the direction of shearing and those oriented perpendicular to the shear plane, and N 2 the difference between normal stresses perpendicular to the shear plane and those in the neutral, traverse, direction 28 . Prior to measurement, the gap error was zeroed at 4 N and gap error calculated as previously described 62 64 .…”
Section: Methodsmentioning
confidence: 99%
“…This represents the normal stress acting in the direction of the shearing/flow. [ 32 ] The higher the value of (τ11τ22), the higher is the melt elasticity. Higher values of (τ11τ22) are due to the higher strength of flow when the molecules are increasingly aligned in the flow direction due to the presence of fibrous nanofillers.…”
Section: Resultsmentioning
confidence: 99%
“…Generally, these stresses occur as a direct result of the fluid motion and are not isotropic. 53 In polymer solutions or melts, the existence of normal…”
Section: Normal Stress Differencesmentioning
confidence: 99%