ライフサイエンスコーパス: tensile stress

1 nds and to challenge their stability against tensile stress.

2 and DSMs) are under intrinsically generated tensile stress.

3 ivisions align with the direction of maximal tensile stress.

4 ell wall network in the direction of maximal tensile stress.

5 s the nuclear membranes against rupture from tensile stress.

6 ear deformation and the magnitude of applied tensile stress.

7 s that rotate towards a direction of maximum tensile stress.

8 n graphene monolayers under tunable uniaxial tensile stress.

9 after a period of plastic deformation under tensile stress.

10 d to high shear stress and some, albeit low, tensile stress.

11 ere they are often subjected to considerable tensile stress.

12 cell type specific expression in response to tensile stress.

13 limited by both the contact duration and the tensile stress.

14 h 600-grit on the surface to be subjected to tensile stress.

15 rate of bond formation or low resistance to tensile stress.

16 developed to predict roof fractures based on tensile stress.

17 and resisted by interleaflet frictional and tensile stresses.

18 ses of articular cartilage to compressive or tensile stresses.

19 min A,C, and histone deacetylation, as these tensile stresses 1) are transmitted to the nucleus throu

20 s (9300 J m(-3) ), extensibility (800%), and tensile stress (2 MPa).

21 pressive buckling should not occur given the tensile stresses across the epidermis.

22 nce of clustering can be imposed by a global tensile stress, although clustering still occurs when is

23 inas without MG have decreased resistance to tensile stress and are softer than controls.

24 considerable physical challenges, including tensile stress and compression.

25 gnificant shifts in yield strength, ultimate tensile stress and ductility.

26 modeling revealed significant reductions in tensile stress and elastic-plastic deformation during di

27 nship between cell density and intercellular tensile stress and forces the tissue into a nonmotile st

28 Membrane deformation upon swelling generates tensile stress and internal pressure, contributing to vo

29 le electrocyclic ring-opening reaction under tensile stress and thus allows us to directly and locall

30 icrotubule arrays, which align along maximal tensile stresses and restrict growth in that direction t

31 cell geometric constraints affect the local tensile stresses and subsequently the three-way feedback

32 ticles reduces glass transition temperature, tensile stress, and modulus of 3D-printed materials.

33 ound inducibility, activation in response to tensile stress, and quantitative expression levels.

34 he contact (ring, or cone cracks), driven by tensile stresses; and "quasi-plastic" mode, a relatively

35 clear deformations typically caused by local tensile stresses are sufficient to cause nuclear membran

36 growth in the sepal can generate transverse tensile stress at the tip.

37 n bi-axial fatigue is attributed to enhanced tensile stresses at the trailing edges of a moving inden

38 sively cross-linked bundles withstood higher tensile stresses before failing.

39 e during continental collision occurs due to tensile stresses built-up between the deep and shallow s

40 embranes demonstrated higher antifouling and tensile stress (by 31%) when compared to pure PES membra

41 Local tensile stresses can also cause nuclear deformations, bu

42 chains to develop along underlying precursor tensile stress chains that gradually strengthen with sub

43 rsial is the experimental finding that large tensile stresses, close to 1 GPa, develop during isother

44 associated threefold decrease in fibrous cap tensile stress compared to untreated controls, estimated

45 chains from the cellulose surfaces under the tensile stress component normal to the macrofibrils can

46 resistance of lithiated Si by lessening the tensile stress concentrations in Si structures.

47 not inconceivable that these localized high tensile stresses could initiate cracks which diverge mon

48 Tensile stress data are measured on PDMS with various su

49 lvular interstitial cells (VIC), whereas the tensile stress deactivated YAP.

50 icrotubules align with the predicted maximal tensile stress direction to guide cellulose biosynthesis

51 ws that microtubules align along the maximal tensile stress direction within the cells, and atomic fo

52 steel and highly tolerant to compressive and tensile stresses due to chemical bonding to the substrat

53 ovides great possibilities for generation of tensile stress during femtosecond laser ablation to roll

54 t notably in plant cells where turgor-driven tensile stresses exceed greatly those observed in animal

55 om passive linear deformation in response to tensile stress exerted by centripetal contraction of the

56 As a second step, we calculated the tensile stress experienced by the cell wall along the fi

57 ly influenced by the ratio of compressive to tensile stresses experienced during each cycle.

58 tion and argued that these are indicative of tensile stress feedback.

59 n of myosin light chain kinase, and enhanced tensile stress fibers.

60 nthesis and alignment in the presence of the tensile stress field generated by a wound contraction pr

61 o nanometric substrate patterning and cyclic tensile stress for 2 days.

62 s, based on the interactions between thermal tensile stress, fracture and ice wedges.

63 ous adhesion failure estimation under cyclic tensile stresses from a resistivity baseline.

64 In highly evolved rifts, tensile stresses from far-field plate motions accumulate

65 The model shows local tensile stresses generated at the interface of the cell

66 In response to the applied tensile stresses, grain boundary sliding takes place whi

67 at its boundary and gradual buildup of high tensile stress has occurred along the dike pathway prior

68 We suggest that tensile stresses imposed by fluid shear stretch endothel

69 ubule alignment along growth-derived maximal tensile stress in adjacent cells would mechanically isol

70 ther supported a contribution of anisotropic tensile stress in division plane orientation.

71 nd differential growth prescribe directional tensile stress in that region, we tested the putative co

72 ls is prevented, the turgor pressure and the tensile stress in the cell wall are reduced by continued

73 ed, resulting in substantial increase of the tensile stress in the lipid bilayer.

74 rface debonding is initiated by the residual tensile stress in the superlayer, and where the interfac

75 micelluloses and lignin co-operate to resist tensile stress in wood.

76 reduction in significant levels of residual tensile stresses in the graphite that are 'frozen-in' fo

77 rtening of the molecule that translates into tensile stresses in the range of several to almost 100 M

78 milar elastic media subjected to an inclined tensile stress, in which stochastic descriptions of mole

79 ve stress drives a growth phenotype, whereas tensile stress increases compaction.

80 irely controlled by electronic factors, with tensile stress inducing stronger binding.

81 pressure to interrogate how compressive and tensile stresses influence valve growth and shape matura

82 and incrementally increasing (i.e. dynamic) tensile stress is an effective tool for dynamically tuni

83 Here tensile stress is created in thin films of potassium (up

84 ng experiments to probe the effects of large tensile stress is difficult.

85 ar stacking of "hard" and "soft" layers, the tensile stress is first accommodated by a large deformat

86 roles in stiffening the cell wall where the tensile stress is high and exposes cells to bursting, an

87 the SAW stress, a second threshold of 8 GPa tensile stress is observed above which the fracture prob

88 p evolution due to in-plane and out-of-plane tensile stresses is validated by photoluminescence (PL)

89 mperature responses suggests compressive and tensile stresses may generate distinct tissue effects wi

90 We suggest, therefore, that water-generated tensile stresses may play a role in living collagen-base

91 to RFUVA, and then subjected to destructive tensile stress measurements.

92 s of electric field (electroporation) and/or tensile stress (mechanoporation) have been used to rever

93 Predictions of localized tensile stress near nanoscale ridges at the metal-film i

94 achieve super-strong mechanical properties (tensile stress of 1.45 MPa, tensile strain of approximat

95 ress so the optimal sample obtained showed a tensile stress of 13.24 +/- 0.76 MPa, which is up to 10

96 modulus is the primary factor affecting the tensile stress of the basic roof beam.

97 The maximum tensile stress of the optimal hybrid construct was 3.42

98 Correspondingly, retinal vessels experienced tensile stress of up to 2.3 kPa near the optic nerve ins

99 Microtubule stretch was negligible up to tensile stresses of approximately 1 MPa.

100 s propose that division plane orientation by tensile stress offers a general rule for symmetric cell

101 ell expansion, and cells divide according to tensile stress on the cell wall.

102 Myosin motors generate both compressive and tensile stresses on F-actin and consequently induce larg

103 Tensile stresses on south polar fractures are expected t

104 Thermal tensile stress perpendicular to the laser scanning direc

105 ganized to align in the direction of maximal tensile stress, presumably reinforcing the local cell wa

106 seful to resist undue circumferential venous tensile stress produced in AV grafting.

107 increasing from 0.45 to 0.5 GPa, the maximum tensile stress reduces by 2.38 MPa.

108 Polymer cold-drawing is a process in which tensile stress reduces the diameter of a drawn fibre (or

109 er, our results demonstrate that compressive/tensile stress regulation of BMP-pSMAD1/5 and MLC2 contr

110 Tensile stress relaxation is combined with transmission

111 ite element modeling is used to evaluate the tensile stresses responsible for the different crack typ

112 attice parameters experience compressive and tensile stresses, significantly splitting the heavy-hole

113 fibers with more OXG content exhibited high tensile stress so the optimal sample obtained showed a t

114 The tensile stress-strain behavior of bone along its longitu

115 The tensile stress-strain curve of bovine bone is modeled us

116 Tensile stress-strain curves and polarization light micr

117 ociation rates as well as high resistance to tensile stress, supporting slow movement of platelets in

118 In this model, we considered the maximum tensile stress tangential to the interfacial surface, as

119 inages in 2011-2013, each of which generates tensile stresses that promote hydro-fracture beneath the

120 In areas of the plant subject to tensile stress, the repression exerted by the negative r

121 muscle cells (SMCs) are exposed to shear and tensile stresses, this study examined the effects of the

122 Above a tensile stress threshold of 6 GPa, fracture of the glass

123 sordered patterns, as well as the buildup of tensile stress throughout the tissue.

124 mechanical stability of nanobeams under high tensile stress to minimize thermal buckling effects, the

125 y deform the nucleus by applying a transient tensile stress to the nuclear membrane.

126 The median values for ultimate tensile stress, ultimate tensile strain, and toughness a

127 stmann hyperelastic material model, ultimate tensile stress, ultimate tensile strain, and toughness o

128 ted in this article is based on the ultimate tensile stress, ultimate tensile strain, and toughness t

129 Mechanical properties, namely, ultimate tensile stress, ultimate tensile strain, and toughness,

130 rrangements, allowing the glass to withstand tensile stresses up to 11 GPa.

131 e arrays remain intact and able to withstand tensile stresses up to temperatures around 370 K.

132 a curving path to a place and time where the tensile stress was insufficient to continue the propagat

133 Residual tensile stresses were calculated for SC and FC specimens

134 m albumin (BSA) resulted in reversible large tensile stresses, whereas MCs with smooth gold surfaces

135 ever bends due to the induced compressive or tensile stresses, which result from the surface free ene

136 n the load-bearing capacity to be diminished tensile stresses within the lower-modulus graded zone, c