A micromechanical basis for partitioning the evolution of grain bridging in brittle materials
By J. W. Foulk, R. Cannon, G. Johnson, Patrick A. Klein, R. O. Ritchie. 2007
622 citations recorded by the source corpus.
Subfields: Ceramics and Composites, Materials Chemistry, Mechanics of Materials
View Paper: https://www.semanticscholar.org/paper/a4d00f327a60a92c2825e177ef49a886419bdb4b
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In Ceramics and Composites
- M. Vandamme
- C. Bobko
- J. A. Ortega
- Jeffrey J. Thomas
- Christine Ortiz
- K. Tai
- Franz-Josef Ulm
- M. Katsnelson
In Materials Chemistry
- Franz-Josef Ulm
- Francisco Guinea
- Wing Kam Liu
- M. Vandamme
- Rodney S. Ruoff
- K. Novoselov
- M. Katsnelson
- V. Shenoy
In Mechanics of Materials
- Franz-Josef Ulm
- M. Vandamme
- Jörn Mosler
- J. A. Ortega
- Wing Kam Liu
- Jeffrey J. Thomas
- C. Bobko
- Otto T. Bruhns
Citations in the corpus
- Gauge fields in graphene (2010, background): “The mechanics of defects of various classes in graphene has been analyzed recently in [69].”
- Anomalous Strength Characteristics of Tilt Grain Boundaries in Graphene (2010, background): “Although a number of studies have been carried out on the mech anics of dislocations and defects in carbon nanotubes [18, 19, 20] and graphene [21], t he mechanical properties of hydrogenfunctionalized graphene [22], as well as the fracture and fa ilure of graphene and carbon nanotubes with multiple”
- a Phase-Field Theory of Dislocation Dynamics, Strain Hardening (2002, methodology): “The distortion field then follows as uk,l = −Gki,l ⋆ (cijmnβ mn),j (6) and the elastic distortion as β kl = −Gki,l ⋆ (cijmnβ mn),j −β kl (7) Finally, the elastic interaction energy Eint is obtained by inserting (7) into the second term of (3).”
- Characteristics of powder metallurgy pure titanium matrix composite reinforced with multi-wall carbon nanotubes (2009, background): “Furthermore, the agglomeration of the bundled CNTs always exists in P/M composite materials because of their van der Waals force, which is attractive or repulsive between carbon atoms [16, 17].”
- Towards variational constitutive updates for non-associative plasticity models at finite strain: models based on a volumetric-deviatoric split (2009, background): “More specifically, every constitutive model falling into th e range of so-called standard dissipative solidsin the sense of Halphen & Nguyen [8] (see also [9]) can be imple ented by applying the aforementioned concept.”
- Hysteresis from Multiscale Porosity: Modeling Water Sorption and Shrinkage in Cement Paste (2015, background): “could instead arise from single-pore effects, due to the molecular nature of water [47, 48], 266 strong electrostatic interactions among dissolved ions and the C–S–H surface [21, 49], and 267 the collapse of the space.”
- Observation of topological valley modes in an elastic hexagonal lattice (2017, background): “Changing of the parity of active devices or modulating of the physical properties in time, for example, has shown to alter the direction and nature of edge waves [7, 8].”
- Statistical indentation techniques for hydrated nanocomposites: concrete, bone, and shale (2007, background): “Figure 1: Conical indentation in a porous material, composed of a solid phase and pore space: (a) matrixporosity morphology; (b) perfectly disordered, polycrystal morphology [adapted from [31]].”
- Microstructural material database for self-consistent clustering analysis of elastoplastic strain softening materials (2018, methodology): “On one hand, analytical approaches, such as rules of mixtures and theoretical micromechanics methods [29, 30, 31, 32, 33], are efficient, but lose accuracy for irregular morphologies and nonlinear history-dependent properties.”