Large amplitude oscillatory shear as a way to classify the complex fluids

By K. Hyun, Sook Heun Kim, K. Ahn, Seung Jong Lee. 2002

808 citations recorded by the source corpus.

Subfields: Cell Biology, Fluid Flow and Transfer Processes, Food Science

View Paper: https://www.semanticscholar.org/paper/1ee161fdf938ab6b503c5619929f45d9eab518b6

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Cell Biology

1. R. Ewoldt
2. G. H. McKinley
3. Seung Jong Lee
4. K. Ahn

In Fluid Flow and Transfer Processes

1. R. Ewoldt
2. G. H. McKinley
3. P. Winter
4. J. Maxey
5. Seung Jong Lee
6. K. Ahn
7. J. Nam
8. S. Egelhaaf

In Food Science

1. R. Ewoldt
2. G. H. McKinley
3. Seung Jong Lee
4. K. Ahn
5. M. Laurati
6. S. Egelhaaf

Citations in the corpus

• Large amplitude oscillatory shear behavior of PEO-PPO-PEO triblock copolymer solutions (2006, background): “Hyun et al. (2002) classified the complex fluids into four types depending on their behavior in the LAOS experiment: type I, strain thinning (G¢, G¢¢ decreasing); type II, strain Fig.”
• Nonlinear rheology of colloidal gels with intermediate volume fraction (2011, background): “…et al. 2006 ; Pham et al. 2006, 2008 and other soft glassy aterials Carrier and Petekidis 2009 ; Cloitre et al. 2000 ; Daniel et al. 2001 ; Heleson et al. 2007 ; Hyun et al. 2002 ; Le Grand and Petekidis 2008 ; Sollich 1998 ; yss et al. 2007 , show a fluidlike response with G 0 and G 1 where 0 2 1.”
• Large amplitude oscillatory shear behavior of complex fluids investigated by a network model: a guideline for classification (2003, methodology): “Schematic diagram of four types of LAOS behavior observed by experiments: (a) type I, strain thinning; (b) type II, strain hardening; (c) type III, weak strain overshoot; and (d) type IV, strong strain overshoot (G0 and G ′′ 0 are moduli in linear region and γ0 is the amplitude at which the moduli b”
• A review of nonlinear oscillatory shear tests: Analysis and application of large amplitude oscillatory shear (LAOS) (2011, methodology): “[62-64] concluded that the LAOS behavior of each class of fluid is closely related to its microstructure.”
• Large amplitude oscillatory shear of pseudoplastic and elastoviscoplastic materials (2010, methodology): “…(e.g. Wilhelm (2002)), Stress decomposition (Cho et al. (2005); Ewoldt et al. (2008); Yu et al. (2009)), computation of viscoelastic moduli (Hyun et al. (2002); Ewoldt et al. (2008)), decomposition into characteristic waveforms (Klein et al. (2007)), and analysis of parameters related to…”
• On secondary loops in LAOS via self-intersection of Lissajous–Bowditch curves (2010, background): “…(e.g. Wilhelm (2002)), Stress decomposition (Cho et al. (2005); Ewoldt et al. (2008); Yu et al. (2009)), computation of viscoelastic moduli (Hyun et al. (2002); Ewoldt et al. (2008)), decomposition into characteristic waveforms (Klein et al. (2007)), and analysis of parameters related to…”
• A new constitutive equation for elastoviscoplastic fluid flows (2007, neutral): “Only G′′ shows an vershoot: this behavior matches the type III of the classification introduced in [8] when using large amplitude oscillatory shear.”