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1 tes in the immediate vicinity of the nearest microcrack.
2 nt matrix, fluid is also squeezed out of the microcrack.
3  for the creation of the new surfaces of the microcrack.
4 resent pores in an aligned clay compact or a microcrack.
5 ess remodelling resulting in accumulation of microcracks.
6 ptions of osteocyte canaliculi around linear microcracks.
7 ity of the bone matrix, and the evolution of microcracks.
8  interaction and coalescence of many tensile microcracks.
9 om 30% to 110% strain without any noticeable microcracks.
10 tural levels, which occurs by the process of microcracking.
11 ly enhanced resistance to contact damage and microcracking.
12 e in permeability is observed, likely due to microcracking.
13  at reducing perforations but may also cause microcrack accumulation, leading to a loss of microstruc
14     We observe reversible planar gliding and microcracking along the (003) plane in a single-crystall
15 d by the coupled poroelastic response of the microcrack and adjacent rock matrix.
16 -ceramics (< 1 microm) showed minimal matrix microcracking and BFS values of [mean (SD) MPa]: M1A = 2
17         Although aspects such as hysteresis, microcracking and so on have to be taken into considerat
18 ed cell attachment and mineralization around microcracks and a higher expression of osteocalcin -an o
19  be lower, thereby limiting the formation of microcracks and minimizing the development of tangential
20                      Microdefects, including microcracks and resorption trenches, may be important co
21                        The geometry of these microcracks and their surrounding elastic stress fields
22 Os, including anisotropic lattice evolution, microcracking, and surface degradation, as a result of w
23 in subchondral bone (SCB) sclerosis, fatigue microcracks, and matrix damage that can progress to para
24 -type cracks as well as inter- and intra-rod microcracks, and that the lengths of these cracks are se
25 d-tissue with no visible damage, tissue with microcracks, and tissue with diffuse damage.
26 ystal-glass thermal mismatches which produce microcracking around larger crystals-agglomerates are as
27       The fraction of leucite particles with microcracks around them, f(mc), was estimated for each p
28 acture energy via deformation mechanisms and microcracks arrest.
29 hical constraint effect and a self-generated microcrack-arresting mechanism.
30 rphyritic andesites, implicating progressive microcracking as the cause of permanent inelastic strain
31 s manifested by the nucleation of many sharp microcracks at the external boundary that rapidly propag
32 Norway, and separates relatively undeformed, microcracked blocks of anorthosite.
33 hod is applied to image key features such as microcracks, carbides, heat affected zone, and dendrites
34  matrix constituents (collagen and mineral), microcrack characteristics, and trabecular architecture
35                                              Microcracks could promote focussed osteoclastic resorpti
36                                          The microcrack cross section is estimated to be 15 um in hei
37 ography, we have fully resolved sequences of microcrack damage as cracks grow under load at temperatu
38  growth involves small-scale, high-frequency microcracking damage localized near the crack tip.
39 lso created weak layers with nanocracking or microcracking damage.
40                                          The microcrack data were subjected to linear regression anal
41 ge and extended cellular processes deep into microcracks, delivering mitochondria to chondrocytes.
42                                          The microcrack densities of four of the six porcelains and t
43                                          The microcrack densities were determined by quantitative ste
44 the magnitude of the increase or decrease in microcrack density after several firings is sufficiently
45 lly significant negative correlation between microcrack density and multiple firings (r2 = 0.15, p =
46 hly significant positive correlation between microcrack density and multiple firings (r2 = 0.24, p =
47 ), was estimated for each porcelain from the microcrack density and the leucite surface area.
48 rcelains that exhibit a measurable change in microcrack density as a function of multiple firings, th
49                                              Microcrack density, leucite particle surface area per un
50 ease crack length with a smaller increase in microcrack density.
51 l dental porcelains could produce changes in microcrack density.
52  measurements presented here show that these microcracks do not permit uniform access to the adjacent
53 : We reconstruct the complete spatiotemporal microcracking dynamics, with micrometer/nanosecond resol
54      We introduce the fabrication and use of microcracks embedded in glass as an optical element for
55 rmation about the potential effect of enamel microcracks (EMCs) on the underlying tooth structures.
56 ng acoustic phonon emissions from individual microcracking events we show that the onset of a seconda
57 or concrete surface, subsequent formation of microcracks exposes the substrate's near-infrared emissi
58 e form of median-type cracks and distributed microcracks, extending preferentially along the boundari
59  greater the UCS, the lower the fines due to microcrack extension.
60 tic mudstones is first observed along planar microcracks, followed by slow penetration into the surro
61                                Moreover, the microcrack formation and extrusion deformation in yarns
62                             During stage II, microcrack formation and particle rupturing accelerate t
63  cycling, with uneven Na(+) distribution and microcrack formation being key contributing factors.
64  thin film and a substrate can notably delay microcrack formation in the film.
65 sures even Na(+) distribution, and mitigates microcrack formation through a pinning effect.
66 thode, which should be maximized to suppress microcrack formation, the main cause of capacity fading
67 e lattice potentially large enough to induce microcrack formation, which are abundant below the hypha
68 eactions, significant phase transitions, and microcrack formation, which lead to considerable interna
69 ial particle-level mechanical stress and the microcracks formation during cycling.
70 nsistent with observations of the closure of microcracks formed parallel to the covalent-sp(2)-bonded
71 T3-E1 mouse osteoblastic cells in biomimetic microcracked hydroxyapatite substrates, differentiated i
72            This study provides evidence that microcracking in dental porcelain can be minimized by a
73 circumferential surface cracking, orthogonal microcracking in laminated sublayers and geometrically c
74  two energy-dissipating mechanisms: multiple microcracking in the outer layers at low mechanical load
75  a dental porcelain influences the degree of microcracking in the porcelain.
76 llographic nucleation and growth of multiple microcracks in abundant poor-deformability microstructur
77   This contraction leads to the formation of microcracks in and around the crystals and the developme
78 l is prone to initiate by the coalescence of microcracks in its polymer matrix.
79  show that the elastic stress around tensile microcracks in three dimensions promotes a mutual intera
80                                       Linear microcracks increased within 10-day loading in diabetic
81                    The fluid build-up at the microcrack indicates that migration out of the rock is h
82                                              Microcracking induced by thermal and mechanical fatigue
83                                          Our microcrack interaction model is based on the three-dimen
84 here is a critical particle size below which microcracking is absent.
85             Collectively, the main effect of microcracks is not to slow down fracture by increasing t
86 results suggest that mineral dissolution and microcracking may have acted in a synergistic way at the
87                               Although teeth microcracks (MCs) have long been considered more of an a
88 nd the microfracture and deformation and the microcrack-microstructure interactions of teeth.
89                    The ultrafast dynamics of microcrack nucleation, growth, and coalescence is inacce
90 captures oriented mesoscale frictional slip, microcrack opening, and splitting with microbuckling.
91 they play a central role in the formation of microcracks or bedding delaminations which ultimately do
92      This "fluid" spontaneously forms mode I microcracks or microanticracks that self-organize via th
93 arying validation accuracy to detect cracks, microcracks, Potential Induced Degradations (PIDs), and
94                  We find that all individual microcracks propagate at the same low, load-independent
95 micro-mechanisms directly by controlling the microcracking rate to slow down the transition in a uniq
96 (P)/V(S) ratio, whose change is related with microcracking, rose from ~1.68 to ~1.8.
97 er perforations but more numerous and larger microcracks than both fracture and non-fracture controls
98  is known about bone microsctructure and the microcracks that are precursors to its fracture, but lit
99  porcelains are often partially encircled by microcracks that are the result of the thermal expansion
100 eposition into subsurface pores, by means of microcracks that connect the pores to the surface.
101                                          The microcracks that form around these leucite particles whe
102 ate the room-temperature brittleness through microcrack tip blunting by layered metallic phase.
103 stress risers leading to the re-formation of microcracks under continued load.
104 itative stereology, whereby intersections of microcracks were counted with a test grid.
105                                       Unlike microcracking, which entails micrometer-level separation
106 g real-world cases, such as shaded areas and microcracks, which were accurately predicted by the syst
107                                              Microcracks within individual enamel rods were also obse
108 is associated with more brittle fracture and microcracks without altering the average length of the c

 
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