viscoelastic fracture
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2021 ◽  
Vol 69 (3) ◽  
Author(s):  
B. N. J. Persson

AbstractWe show that the Persson-Brener theory of crack propagation in viscoelastic solids gives a viscoelastic fracture energy factor $$G/G_0 = 1+f$$ G / G 0 = 1 + f which is nearly the same as the viscoelastic factor obtained using the cohesive-zone model. We also discuss finite size effects and comment on the use of crack propagation theories for “solids” with a viscoelastic modulus that vanishes at zero frequency. Graphical Abstract


2021 ◽  
Author(s):  
Bo Persson

Abstract We show that the Persson-Brener theory of crack propagation in viscoelastic solids gives a viscoelastic fracture energy factor G/G0 = 1 + f which is nearly the same as the viscoelastic factor obtained using the cohesive-zone model. We also discuss finite-size effects and comment on the use of crack propagation theories for “solids” with a viscoelastic modulus that vanishes at zero frequency.


Polymers ◽  
2019 ◽  
Vol 11 (8) ◽  
pp. 1291 ◽  
Author(s):  
Xiaoxi Yu ◽  
Yuan Li ◽  
Yuquan Liu ◽  
Yuping Yang ◽  
Yining Wu

Viscoelastic surfactant (VES) fluid and hydrolyzed polyacryamide (HPAM) solution are two of the most common fracturing fluids used in the hydraulic fracturing development of unconventional reservoirs. The filtration of fracturing fluids in porous media is mainly determined by the flow patterns in pore-throat structures. In this paper, three different microdevices analogue of porous media allow access to a large range of Deborah number (De) and concomitantly low Reynolds number (Re). Continuous pore-throat structures were applied to study the feedback effect of downstream structure on upstream flow of VES fluid and HPAM solution with Deborah (De) number from 1.11 to 146.4. In the infinite straight channel, flow patterns between VES fluids and HPAM solution were similar. However, as pore length shortened to 800 μm, flow field of VES fluid exhibited the triangle shape with double-peaks velocity patterns. The flow field of HPAM solution presented stable and centralized streamlines when Re was larger than 4.29 × 10−2. Additionally, when the pore length was further shortened to 400 μm, double-peaks velocity patterns were vanished for VES fluid and the stable convergent flow characteristic of HPAM solution was observed with all flow rates.


Soft Matter ◽  
2018 ◽  
Vol 14 (30) ◽  
pp. 6386-6392 ◽  
Author(s):  
Quang D. Tran ◽  
Marcos Marcos ◽  
David Gonzalez-Rodriguez

Interstitial flow induces deformation and fracture in a model tumor.


2017 ◽  
Vol 205 (1) ◽  
pp. 37-56 ◽  
Author(s):  
Berangere Doll ◽  
Hasan Ozer ◽  
Jose J. Rivera-Perez ◽  
Imad L. Al-Qadi ◽  
John Lambros

Author(s):  
N. J. Balmforth ◽  
R. V. Craster ◽  
I. J. Hewitt

Steady rucks in an elastic beam can roll at constant speed down an inclined plane. We examine the dynamics of these travelling-wave structures and argue that their speed can be dictated by a combination of the physical conditions arising in the vicinity of the ‘contact points’ where the beam is peeled off the underlying plane and stuck back down. We provide three detailed models for the contact dynamics: viscoelastic fracture, a thermodynamic model for bond formation and detachment and adhesion mediated by a thin liquid film. The results are compared with experiments.


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