ライフサイエンスコーパス: plastic deformation

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

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

3 xceptionally high rates of cross slip during plastic deformation.

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

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

6 ed crystals demonstrate dislocation-mediated plastic deformation.

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

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

9 19' martensite transformation are induced by plastic deformation.

10 to shear sliding of molecular layers during plastic deformation.

11 e lattice softening in response to extensive plastic deformation.

12 uggestive of a universal mode of cooperative plastic deformation.

13 c materials to achieve high ductility during plastic deformation.

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

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

16 ameters that govern superlattice elastic and plastic deformation.

17 ries as they gradually lose coherency during plastic deformation.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

35 We observe plastic deformation attributable to the migration and re

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

58 The overall plastic deformation includes local plastic slip events t

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

74 Plastic deformation of materials occurs by the motion of

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

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

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

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

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

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

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

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

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

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

85 atmosphere of differential pressure without plastic deformation or fracture.

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

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

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

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

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

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

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

93 Comparison of the plastic deformation resulting from controlled compressio

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

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

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

97 rication of stable nanomaterials with severe plastic deformation techniques.

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

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

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

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

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

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

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

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

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

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

108 Plastic deformation via structural transitions has never

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

110 The plastic deformation was confirmed in microscopic images

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

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

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

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