ライフサイエンスコーパス: plastic deformation

1 compared with the contralateral normal eyes (plastic deformation).

2 as well as increased material stiffness and plastic deformation.

3 ions and twinning are the main mechanisms of plastic deformation.

4 t set of AK structures were interpreted as a plastic deformation.

5 ries as they gradually lose coherency during plastic deformation.

6 esting that slip on (100) or (110) dominated plastic deformation.

7 dentation test is indicative of the onset of plastic deformation.

8 xceptionally high rates of cross slip during plastic deformation.

9 mediately takes over as the dominant mode of plastic deformation.

10 of twin boundaries leading to large uniform plastic deformation.

11 calized amorphization and contributes to the plastic deformation.

12 ed cytoarchitectures that are susceptible to plastic deformation.

13 e exceeded its elastic strain limit, causing plastic deformation.

14 , whereas the skin region could undergo more plastic deformation.

15 w dislocations playing an important role for plastic deformation.

16 ons for improving metal processing by severe plastic deformation.

17 oAl grains with thick GBs, which accommodate plastic deformation.

18 circuit and an amorphous material undergoing plastic deformation.

19 gas intrusion, which initially grows through plastic deformation.

20 agment with no detectable partial rupture or plastic deformation.

21 mperature (Tg), by subjecting them to active plastic deformation.

22 osslinked by weak bonds usually exhibit more plastic deformation.

23 ameters that govern superlattice elastic and plastic deformation.

24 ucture of disordered colloidal solids during plastic deformation.

25 to the beta-sheets, which marks the onset of plastic deformation.

26 ed crystals demonstrate dislocation-mediated plastic deformation.

27 tion layer, confirming the effects of severe plastic deformation.

28 , whereas the wild-type cells show much less plastic deformation.

29 19' martensite transformation are induced by plastic deformation.

30 to shear sliding of molecular layers during plastic deformation.

31 e lattice softening in response to extensive plastic deformation.

32 uggestive of a universal mode of cooperative plastic deformation.

33 c materials to achieve high ductility during plastic deformation.

34 tallic glass it responds with elastic and/or plastic deformations.

35 mics show subsurface cone fracture and quasi-plastic deformation above critical loads P(C) (cracking)

36 nanowires are also found to exhibit elastic-plastic deformation accompanying the martensitic transfo

37 hich describes the increase in strength with plastic deformation, affects fracture toughness and duct

38 The solid network's plastic deformation also manifests creep and yield regim

39 two different energy dissipation mechanisms: plastic deformation and acoustic wave attenuation.

40 dislocation climb plays a unique role in the plastic deformation and creep of crystalline materials.

41 ar dynamics simulations reveal predominantly plastic deformation and densified region formation by th

42 At high temperature the plastic deformation and ductile flow is meditated by the

43 PVDF films underwent significant plastic deformation and extensive crystal fragmentation,

44 t nucleation and evolution mechanisms during plastic deformation and failure at the mesoscales.

45 ther aggravated due to bending-induced local plastic deformation and Li-filaments pulverization.

46 cations, are central to the understanding of plastic deformation and mechanical strength, as well as

47 stigated the effects of alloying elements on plastic deformation and microstructure evolution in poly

48 t high temperatures, thus enabling glasslike plastic deformation and reprocessing without depolymeriz

49 A new mechanism of plastic deformation and stress relaxation at high strain

50 lagen organization between tendons loaded to plastic deformation and subsequent structural relaxation

51 trix were refined by high-temperature severe plastic deformation and, subsequently, a new alloy compo

52 rough coherent precipitates and thus produce plastic deformation), and we envisage that this lattice

53 tiple manufacturing steps including casting, plastic deformation, and heat treatment to achieve the d

54 bject to oscillatory shear near the onset of plastic deformation, and of the period bifurcation casca

55 Dislocations are the primary drivers of plastic deformation, and their interactions with each ot

56 NIL processes, Mac-Imprint does not rely on plastic deformation, and thus, it allows for replicating

57 t the lattice level, the basic mechanisms of plastic deformation are twinning (whereby crystallites w

58 These results establish plastic deformation as a versatile knob for the manipula

59 the rejuvenated BMG resulted in homogeneous plastic deformation as was evident from the high strain

60 attrition, and inconsistent with fracture or plastic deformation, as shown using direct imaging.

61 solutes' atomic neighborhoods more prone to plastic deformation at an increased critical stress.

62 al distortions, causing the proliferation of plastic deformation at structurally weak regions.

63 entary rock undergoing penetrative, (visco-) plastic deformation at the critical state".

64 Friction-assisted plastic deformation at the joint interface is essential

65 ely elastic deformations at low pressures or plastic deformations at high pressures.

66 collagen requires energy to be absorbed by "plastic" deformation at higher structural levels, which

67 We observe plastic deformation attributable to the migration and re

68 imulation demonstrated that the variation in plastic deformation behavior is correlated with local at

69 We present investigations on the plastic deformation behavior of a brittle bulk amorphous

70 critical to understanding and analyzing the plastic deformation behavior of omega-Zr or mixed alpha-

71 This crossover indicates a transition in the plastic deformation behaviour from three-dimensional ran

72 noscale wear mechanisms include fracture and plastic deformation, but recent experiments and models p

73 commodates tensile strains up to 60% without plastic deformation by aligning BNNTs, which enhances th

74 ger hcp phase progressively increases during plastic deformation by forming at the stacking-fault net

75 entered cubic iron that had undergone severe plastic deformation by mechanical milling.

76 This plastic deformation can be precisely controlled by using

77 mbined with grain orientation, c/a ratio and plastic deformation can result in characteristic twin bo

78 Plastic deformation, degradation, and relaxation of stre

79 rowth, the nanocontacts exhibit only limited plastic deformation despite high applied stresses.

80 e find that hydrogen charged specimens after plastic deformation display a very characteristic patter

81 leation is essential to our understanding of plastic deformation, ductility, and mechanical strength

82 ecipitates also significantly affected local plastic deformation during compression, with their influ

83 Visco-plastic deformation during cooling was found to be depen

84 ant reductions in tensile stress and elastic-plastic deformation during dicing, thanks to a lower CoF

85 rrific mechanical integrity that resists the plastic deformation during the lithiation/delithiation.

86 ture of the nuclear envelope and for nuclear plastic deformation during transmigration through small

87 eds during MSGL formation is accommodated by plastic deformation, facilitated by continuous sediment

88 Twinning is an essential mode of plastic deformation for achieving superior strength and

89 Twinning on the plane is a common mode of plastic deformation for hexagonal-close-packed metals.

90 However, for materials undergoing plastic deformation, fracture, and damage, the correspon

91 ures crystal defects in materials undergoing plastic deformation, generating vast datasets with high

92 r bands, even in locations where significant plastic deformation had occurred, showing that plastic s

93 s in sapphire introduced by high-temperature plastic deformation has been investigated with the use o

94 ng the shear-sliding process, reflecting the plastic deformation has fractal structure at the tempera

95 Time dependent plastic deformation in a single crystal nickel-base supe

96 ations in a crystal is the key mechanism for plastic deformation in all materials.

97 he significance of vacancies in facilitating plastic deformation in B(4)C and suggests a potential st

98 Plastic deformation in ceramic materials is normally onl

99 For instance, some BMGs exhibit significant plastic deformation in compression or bending tests, but

100 Plastic deformation in crystalline materials consists of

101 as dislocation multiplication, controls the plastic deformation in crystals beyond their elastic lim

102 Plastic deformation in crystals is mediated by the motio

103 ted the limitations of using pure elastic or plastic deformation in explaining the results.

104 ale molecular simulations reveal that active plastic deformation in glassy polymers, at temperatures

105 shear bands, which are a key feature of the plastic deformation in MGs.

106 arge scale molecular dynamics simulations of plastic deformation in nanocrystalline aluminum with mea

107 during grain growth, recrystallization, and plastic deformation in nanocrystalline materials.

108 amorphous phase, which was mainly driven by plastic deformation in solid state introduced by ultraso

109 mentally different avenues for accommodating plastic deformation in the body-centered cubic (bcc) var

110 Supercrystals accommodate plastic deformation in the form of pile-ups, dislocation

111 tions indicate that isolated dimers induce a plastic deformation in the lipid bilayer, which is parti

112 This zone may arise from low-strain plastic deformation in the matrix between the bands.

113 While plastic deformation in this alloy is usually dominated b

114 ilm further established the explicit role of plastic deformation in this newly reported sub-Tg solid-

115 The overall plastic deformation includes local plastic slip events t

116 d process essential to many phenomena during plastic deformation, including dislocation pattern forma

117 fluorescence emerge with the accumulation of plastic deformation, indicating that in these polymeric

118 Here we show that plastic deformation induces robust magnetism in the quan

119 ional changes of crystal dislocations during plastic deformation influence the mechanical properties

120 atomic-scale planar deformation faulting in plastic deformation introduces a different approach for

121 Plastic deformation introduces large numbers of dislocat

122 Moreover, the plastic deformation is a constant fraction of the total

123 Here, failure with plastic deformation is already observed under static loa

124 However, irrespective of grain size, plastic deformation is considered irrecoverable.

125 causes that a portion of energy expended on plastic deformation is dissipated and the rest is stored

126 Dislocation-mediated plastic deformation is expected to become inactive below

127 a stress-free state after shear deformation, plastic deformation is observed only with unbinding.

128 The propagation of the plastic deformations is mainly affected by the Young's m

129 oad without any irreversible damage (such as plastic deformation), it is usually brittle and can fail

130 art of the sp(2)-to-sp(3) transition enables plastic deformation, leading to a large fracture strain

131 Here we determine directly the elastic and plastic deformation mechanism of iron at pressures of th

132 titatively reveal the switch of the dominant plastic deformation mechanism with grain size and the re

133 cteristics of the wave propagation behavior, plastic deformation mechanisms (dislocation nucleation,

134 materials reveal low wear rates, yet, their plastic deformation mechanisms also influence their wear

135 f intragranular dislocation sources leads to plastic deformation mechanisms that substantially differ

136 rmal stress exceeds the yield stress undergo plastic deformation mediated by GND activations.

137 ctional forging (MDF) as a well-known severe plastic deformation method.

138 lex relationships between alloying elements, plastic deformation, microstructural evolution, and mate

139 ch phase transformation offers an additional plastic deformation mode comparable to twinning.

140 ntation testing to explore the dependence of plastic deformation modes on the thickness of CuZr layer

141 brittle deformation in the shallow crust and plastic deformation near the Moho.

142 Plastic deformation occurred by slip along {110} <1[Form

143 In crystalline materials, plastic deformation occurs by the motion of dislocations

144 ct evidence for the mechanism underlying the plastic deformation of a nanowire.

145 It is known that the room-temperature plastic deformation of bulk metallic glasses is compromi

146 Plastic deformation of crystalline materials with isotro

147 wing that increases in strain facilitated by plastic deformation of Earth's crust during the earthqua

148 with dislocations, is critically required in plastic deformation of hexagonal close-packed crystals a

149 Twinning is commonly activated in plastic deformation of low stacking-fault face-centered

150 fect and its importance in understanding the plastic deformation of materials at the submicron scale.

151 Plastic deformation of materials occurs by the motion of

152 intricate interplay during room-temperature plastic deformation of model nanocrystalline Al microstr

153 e discuss how the effects of the elastic and plastic deformation of molecular crystals on the diffrac

154 perimentally and theoretically to govern the plastic deformation of nanocrystals over a material-depe

155 of reoriented martensite accompanied by the plastic deformation of Nb-rich phase and lamellar NiTi-N

156 alysis of a variety of parameters related to plastic deformation of the crystalline materials when at

157 mpliance required for even simple elastic or plastic deformation of the device.

158 hat orthopyroxene may play a key role in the plastic deformation of the lithosphere in a critical tem

159 ghening are the resulting crack bridging and plastic deformation of the metallic particles, together

160 lar, the GLLO method significantly mitigates plastic deformation of the PI film and minimizes carbona

161 IV) B19' martensitic transformation, and (V) plastic deformation of the specimen.

162 critical role of dislocation interactions in plastic deformation of thin films and can be readily gen

163 variant temperatures and strain rates during plastic deformation of Zr-based bulk metallic glass (BMG

164 es by considering the effects of elastic and plastic deformations of the fractal asperities.

165 mography, we document the effects of crystal-plastic deformation on atomic-scale elemental distributi

166 atmosphere of differential pressure without plastic deformation or fracture.

167 ass-revealing a complex dance of elastic and plastic deformations, phase transitions, and their inter

168 They are known to accommodate plastic deformation primarily through their migration, w

169 Simulation results reveal that plastic deformation proceeds by the nucleation of partia

170 These preinjected defects enabled the plastic deformation process of the ceramics at room temp

171 to their mechanical properties, even though plastic deformation processes in the interiors of planet

172 through higher tablet hardness and increased plastic deformation profiles of the post-milled powders,

173 They are produced during cold work plastic deformation, quenching experiments or under irra

174 es including pulsed electrodeposition (PED), plastic deformation, recrystallization, phase transforma

175 In contrast, severe plastic deformation reduces the LCO towards random SS.

176 e recovered slightly, but a relatively large plastic deformation remained.

177 ic glasses (BMGs) was reported to facilitate plastic deformation, rendering BMGs more ductile at room

178 In metallic nanostructures, plastic deformation requires higher stresses than those

179 Comparison of the plastic deformation resulting from controlled compressio

180 slocation cross-slip from the early stage of plastic deformation, resulting in strong dislocation int

181 The onset of plastic deformation reveals itself as a repetitive jump

182 ll documented with the development of severe plastic deformation (SPD) for improving the physical and

183 ignificantly altered via changing the severe plastic deformation (SPD) processing pathway.

184 gnificant complications in the mechanisms of plastic deformation, strengthening, and ductility, and t

185 igh pressure torsion (HPT) one of the severe plastic deformation techniques which provides an opportu

186 rication of stable nanomaterials with severe plastic deformation techniques.

187 The effect decreases the plastic deformation temperature of B(4)C by 200 degrees

188 t is able to produce a much larger amount of plastic deformation than that in FCC pillars.

189 omplete shape recovery is due to an additive plastic deformation that displays the same power-law dyn

190 d length in the protein mechanophores during plastic deformation that is preserved after the recovery

191 induces large crystallographic rotations and plastic deformation that physically heal the cracks.

192 ting the equiatomic CrMnFeCoNi HEA to severe plastic deformation through swaging followed by either q

193 disordered phases revealed a transition from plastic deformation to brittle failure and at least a fa

194 llular response from (visco-)elastic through plastic deformation to cell structural failure and show

195 d is estimated from the propagation depth of plastic deformations to a value of approximately 750-800

196 ounced softening under extension, a possible plastic deformation transition under radial compression,

197 A fundamental understanding of the elastic-plastic deformation transition, in particular, incipient

198 Despite the glassy regime, the bulk plastic deformation triggered the requisite molecular mo

199 ated area shows that there is no appreciable plastic deformation under a 4 nm groove, confirming that

200 undergoes brittle cleavage after a period of plastic deformation under tensile stress.

201 slip on planes near (100) and (110) dominate plastic deformation under these conditions.

202 Here we show that plastic deformation under triaxial compression at room t

203 bimetal nanocomposite synthesised via severe plastic deformation uniquely possesses simultaneous high

204 Plastic deformation via structural transitions has never

205 transformations, where the energy barrier to plastic deformation (via lattice-invariant shears, as in

206 The plastic deformation was confirmed in microscopic images

207 ral low-IOP normal eyes (hypercompliant plus plastic deformation) were more than eight times greater

208 n be an efficacious mechanism to accommodate plastic deformation when the grain size of polycrystalli

209 e contribution of recoverable deformation to plastic deformation, which impacts the rate at which yie

210 Cu was blunted by dislocation-slip mediated plastic deformation, while the cracks in the UFG Cu were

211 r undergo structural collapse or significant plastic deformation with a reduction in compressive stre

212 On Earth, fracturing gives way to crystal-plastic deformation with increasing depth resulting in a

213 daries (TBs) are able to sustain substantial plastic deformation without fracture due to shear-induce