ライフサイエンスコーパス: buckle

1 traocular lens, glaucoma implant, or scleral buckle).

2 ed using an encircling element and segmental buckle.

3 nd the MTs within the leading process become buckled.

4 ilar to graphene but with varying degrees of buckling.

5 o estimate the load they can transmit before buckling.

6 ptimized to transmit the largest load before buckling.

7 uctures, many strategies are used to prevent buckling.

8 e epithelium-stroma area mismatch leading to buckling.

9 ith cryotherapy and more extensive segmental buckling.

10 ckward toward their minus ends, resulting in buckling.

11 e, such as solitons, breathers and localised buckling.

12 ucture, are prone to substantial bending and buckling.

13 ip-localized, decaying, and short-wavelength buckling.

14 4A ROP in the right eye and received scleral buckling.

15 multiple scales of anisotropic, out-of-plane buckling.

16 gnetic systems break the symmetry before the buckling.

17 ures into extended 3D layouts by compressive buckling.

18 rom limited curvature and the possibility of buckling.

19 rize conditions for bead movement and bundle buckling.

20 , such as nonlinear transduction and dynamic buckling.

21 eft eye rhegmatogenous RD treated by scleral buckle 1 month after the last IAC and cataract surgery 1

22 The feasibility of using buckled 2D Te for ultrastretchable strain sensors with a

23 s plana vitrectomy (PPV), encircling scleral buckle, 360 degrees Laser endophotocoagulation, and sili

24 ted with PPV coupled with encircling scleral buckle, 360 degrees laser retinopexy and silicon oil tam

25 ctomy (88%), combined vitrectomy and scleral buckle (8%), and encirclement (3%).

26 ormed under contractile load into sinusoidal buckles, a behavior dependent on posttranslational "dety

27 olds, period-doubles, ridges and delaminated-buckles according to their distinctive topographical cha

28 ngth, as demonstrated by outward sliding and buckling after ablation-mediated release from the centro

29 Initial surgery using scleral buckling alone was performed in most (8 of 13, 62%) of t

30 derwent PPV combined with encircling scleral buckle and 360 degrees laser retinopexy of the periphera

31 , followed by laser barricade (23%), scleral buckle and pneumatic retinopexy (both 11%), and cryother

32 rectomy (PPV; 15 patients), combined scleral buckle and PPV (4 patients), pneumatic retinopexy (3 pat

33 Scleral buckle and PPV/SB were superior to PPV for SSAS (P = 0.0

34 Scleral buckle and vitrectomy combined with belt buckle were per

35 gs of 62% and 60.8% when compared to scleral buckle and vitrectomy, respectively.

36 tential cost savings comparing PR to scleral buckle and vitrectomy.

37 t into two branches under tensile strain-low buckled and high buckled structures, which respectively

38 , the latter two modes are associated with a buckled and propeller-twisted geometry of the basepair.

39 anoscale pores driven by twisting, rotation, buckling and bending of pore walls contributes to the la

40 At birth, SMC contraction drives inner layer buckling and centripetal displacement to occlude the art

41 m a competition between the strain energy of buckling and chemical energy of electronic hybridization

42 clinical use due to several limitations: 1- buckling and compression effects in the shaft and needle

43 of collagen network mechanics, such as fiber buckling and cross-link rupture, and reduces the overall

44 try-breaking transitions associated with the buckling and folding of curved multilayered surfaces-whi

45 Thin-film buckling and nanoindentation are used to evaluate the me

46 interacting Au is nonplanar with significant buckling and numerous polymorphs as in vacuum, whereas o

47 be a specimen support design that eliminates buckling and reduces electron beam-induced particle move

48 mantle and deformation associated with slab buckling and stagnation.

49 We show that this movement is caused by buckling and subsequent deformation of the suspended ice

50 how induced magnetic interactions affect the buckling and the configuration of magnetoelastic membran

51 Stresses are relaxed by both out-of-surface buckling and the emergence of defects in the quasi-hexag

52 al techniques, including vitrectomy, scleral buckle, and pneumatic retinopexy, are the only means to

53 lar the tendency of the interdomain hinge to buckle, and then we apply an external force onto the con

54 elusive how actin filaments are reoriented, buckled, and bundled as well as undergo tension buildup

55 a distribution of 83% vitrectomy, 5% scleral buckling, and 12% pneumatic retinopexy in 2014.

56 easingly looking to harness the deformation, buckling, and failure of soft materials for functionalit

57 kle is categorized into three modes-bending, buckling, and sliding.

58 components, we found that biofilms deform by buckling, and that adhesion transmits these forces to th

59 cal responses--such as bending, twisting and buckling--and on local-feature development (primarily re

60 The buckling approach is generally applicable to a wide rang

61 The delamination buckling approach provides a facile means to dynamically

62 er, it remains unknown how bundle length and buckling are controlled by external physical factors.

63 eak forces were shown to create an efficient buckle as in a hook-and-loop fastener, and fine structur

64 act with the cortex, the astral microtubules buckle as they exert compressive, pushing forces.

65 We observe buckling, axial contraction, failure, and total static s

66 tigate the mechanical dynamics of individual buckling beams, cooperative coupling among neighbouring

67 Scissoring in thick bars suppresses buckling behavior in serpentine traces that have thickne

68 leave a distinct signature in the nonlinear buckling behavior of a cellular material built out of el

69 the surrounding cytoplasm and MAP tau on MT buckling behavior, which allows MT filaments to bear muc

70 As for the buckling behaviors, a significant enhancement could be o

71 izes the intrahelical base primarily through buckling both surrounding base pairs.

72 on of the continuum model, we analyze tissue buckling by a line tension applied along a circular cont

73 we illustrate that concurrent wrinkling and buckling can actually occur and be directly simulated.

74 he surface undulation and overall structural buckling, can all be predicted in a straightforward mann

75 superelastic conducting fibers, comprising a buckled carbon nanotube sheath on a rubber core, are fab

76 these hair-like-diameter fibers, comprising buckled carbon nanotube sheaths on a rubber core, can be

77 n dynamics and lasing properties in a single buckled CdS nanoribbon (NR) by strain-engineering.

78 In addition, we also present the lasing of buckled CdS NRs, in which the strain-dominated mode sele

79 extensively remodel epithelia driving tissue buckling, closure and extension.

80 Continuum mechanics models suggest that buckled cofilactin filaments localize elastic energy at

81 lysis rates for each protomer, such that the buckled conformation favors ATP hydrolysis.

82 We demonstrate that the magnetoelastic buckling corresponds to a classical Landau second-order

83 Scleral buckling declined from 6502 procedures in 2000 to 1260 p

84 and finite element analyses reveal that the buckling deformation of the outer spherical shell domina

85 s with history of retinoblastoma and scleral buckling developing tractional RD.

86 To locally control the buckling direction, masks with holes were used to guide

87 ling step with different masks to encode the buckling directions of separate domains.

88 ne tension decreases, protrusion resumes and buckling disappears, until the next cycle.

89 e compression on the flagellar bundle causes buckling, disassembly and reorganization on the other si

90 l transformation that forms multiple ordered buckling domains separated by distorted domain boundarie

91 licone oil tamponade with or without scleral buckle, drainage retinotomy, or relaxing retinectomy.

92 slow or blocked, the pore opens by membrane buckling, driven by the line tension acting on the detac

93 ugh-thickness gradient and thus directed the buckling during the subsequent unmasked swelling process

94 model can account semiquantitatively for the buckling dynamics of both DNA and RNA.

95 ed snake muscle activation patterns and body-buckling dynamics reproduced the observed patterns, sugg

96 nder high tensile stress to minimize thermal buckling effects, therefore keeping control of the nanom

97 attributes, including complete pre- and post-buckling elasticity, outstanding electrical conductivity

98 crocoils formed by deterministic compressive buckling establish the basis for systems that can offer

99 Buckling events, which occur due to compressive intracel

100 riations in expansion rate that induce local buckling events.

101 ytical and numerical calculations as well as buckling experiments performed on two- and three-dimensi

102 na vitrectomy (1/19, 5.3%), and post-scleral buckle exposure (1/19, 5.3%).

103 uctures driven by the magnetic force-induced buckling, fabricating multistate electrical switches for

104 l severing at actin-cofilactin boundaries of buckled filaments is more prominent than predicted by co

105 s induces cargo crowding and inward membrane buckling, followed by constriction of the nascent bud ne

106 ion and extension leads to a decrease in the buckling force that we attribute to the bundle remaining

107 Buckling forces physically distort the shape of the morp

108 bundling increases the frequency of filament buckle formation, consistent with a requirement of accel

109 design tools for predicting both wrinkle and buckle formations.

110 different folding mechanisms such as tissue buckling from mechanical stress, axon tethering, localiz

111 rough designing and introducing a controlled buckled geometry in its intriguing chiral-chain lattice.

112 th an S-like shape that exhibit a non-planar buckled geometry, with the handedness of the substrate's

113 These buckles grew approximately 3.4-fold faster than the diff

114 institution before referral, or if a scleral buckle had been placed.

115 s and examined a known compound, BaSn2, with buckled hexagonal layers.

116 as developed, introducing the concept of the buckling hinge.

117 icene, a silicon analogue of graphene, has a buckled honeycomb lattice and, because of its Dirac band

118 d[Formula: see text]m phase at 500 GPa forms buckled honeycomb layers that give rise to a Dirac cross

119 ing magnetoelectric characteristics of these buckled-honeycomb lattice materials.

120 plate; (ii) the emergence of a contact layer buckled in an ice-like manner; and (iii) nucleation on c

121 We show how simple analysis of viscous buckles in ice-penetrating radar data can quantify the s

122 The atomic buckling in 2D "Xenes" (such as silicene) fosters a plet

123 2.5 diopter) were caused by previous scleral buckling in one case and by keratoconus in the other cas

124 ght asymmetries at the poles, which bias the buckling in opposite directions, thus leading to a helic

125 nto sinusoidal patterns via cooperative beam buckling in response to an electrochemically driven sili

126 in BD can be effectively treated by scleral buckling in selected cases and PPV in more complex cases

127 nalytical treatment are developed to examine buckling in stationary (pinned) and moving swimmers.

128 We find that collective fiber buckling in the vicinity of a local active unit results

129 modeling of pre-twisted beams in bending and buckling indicates that the different growth tactics of

130 orneal astigmatism in keratoconus or scleral-buckle-induced regular astigmatisms can be equally well

131 tation in two cases - a patient with scleral-buckle-induced regular corneal astigmatism and a patient

132 ic IOL implantation in patients with scleral-buckle-induced regular corneal astigmatism.

133 der quasi-static compression, and arise from buckling-induced kink-antikink bands that provide domain

134 ol 3D configurations of micro- and nanoscale buckling-induced kirigami structures.

135 cutting geometry, it is shown that distinct buckling-induced out-of-plane configurations can be obta

136 characterization of thin films experiencing buckling-induced out-of-plane shape transformations and

137 esults suggest a mechanism wherein nanoscale buckling instabilities can define the global topology of

138 In addition to the separate wrinkling and buckling instabilities developed under their respective

139 ervations of uniflagellar bacteria show that buckling instabilities of the hook protein connecting th

140 al lipids can act synergistically to trigger buckling instability and achieve extreme constriction.

141 lms during compression reveal an interfacial buckling instability followed by folding, which is in go

142 embranes of pre-twisted kagome lattices, the buckling instability is avoided, allowing for smooth and

143 egrees "flicks," the latter resulting from a buckling instability of the flagellum.

144 In its simplest form the magnetoelastic buckling instability refers to the sudden bending transi

145 lar focus on the parameter dependence of the buckling instability.

146 s to map out the parameter dependence of the buckling instability.

147 the midpiece section, likely arising from a buckling instability.

148 drives the collapse and initiates a dynamic buckling instability.

149 le shape deformation that causes the rods to buckle into banana-shaped particles.

150 eved through mechanical instabilities (i.e., buckling) introduced by structural hierarchy and retaine

151 ducing coordinated protrusive forces without buckling is not well understood.

152 Buckling is predicted to enhance cofilactin filament sev

153 mechanism from the rod instability to shell buckling is shown to explain the nonmonotonic variation

154 location, squeezing the tube with or without buckling it locally.

155 Finally, we show that Li whiskers can yield, buckle, kink or stop growing under certain elastic const

156 aws and scales found in nature, we show that buckling kirigami structures applied to footwear outsole

157 ly to have the repair performed with scleral buckle, laser barricade, and pneumatic retinopexy.

158 al properties are greatly diversified by the buckled lattice structure, stacking configuration, intra

159 pological insulators, the monolayer (ML) low-buckled (LB) mercury telluride (HgTe) and mercury seleni

160 Scleral buckling leads to short-term decreased endothelial cell

161 s reduced, MTs uncoupled from sarcomeres and buckled less during contraction, which allowed sarcomere

162 the interactions of single molecules with a buckled lipid bilayer.

163 Quantifying the buckling magnitude with subangstrom precision is, howeve

164 Our insights into buckling mechanisms provide the bases to develop soft, a

165 on is dominated by either sarcomeric-like or buckling mechanisms.

166 quantify shape and stress-strain relation of buckled membranes, we demonstrate that gel phase bilayer

167 Under certain conditions, the buckling microtubules self-organize into parallel bendin

168 such that compression activates a series of buckling modes that reorient the head and scramble its e

169 s, which respectively lead to a low and high buckled monolayer structure.

170 Slender filaments bend and buckle more easily than stretch.

171 d peripheral laser ablation (n = 3), scleral buckle (n = 2), pars plicata vitrectomy (n = 2), and no

172 semiconductors, such as dichalcogenides and buckled nanomaterials with sizeable bandgaps.

173 pectral characteristics of broad emission of buckled NR, which can be understood by the discrepancy o

174 we develop a new method to fabricate uniform buckled NRs supported on polydimethylsiloxane (PDMS).

175 accompanying with the macro vibration, micro buckles occur on the interfaces of the delamination with

176 The buckling occurs between the front of the lamellipodium,

177 zes the critical flexibility number at which buckling occurs.

178 ly of such systems via controlled mechanical buckling of 2D precursors built on shape-memory polymer

179 ysis is validated by uniaxial compression to buckling of 3D printed biomimetic rods using a polymeric

180 distribution of outcrop forces following the buckling of few strands.

181 we show a versatile approach to control the buckling of individual domains and thus the outcome conf

182 driven or followed by bending, looping, and buckling of MT filaments.

183 nobserved in other Hsp90 homologs, is due to buckling of one of the protomers and is most pronounced

184 deformation profiles that drive out-of-plane buckling of planar films into predictable 3D shapes.

185 parameters to [Formula: see text] but larger buckling of planes.

186 ere, we demonstrate on-demand reconfigurable buckling of poly(N-isopropylacrylamide-co-acrylic acid)

187 that structures that reduce or eliminate the buckling of the [Formula: see text] planes could have an

188 severe distortions that are reflected in the buckling of the anthracene framework and dislocation of

189 red to other LnAuZ phases as a result of the buckling of the Au-Sb honeycomb layers to create interla

190 airs at the periphery of anthracene leads to buckling of the backbone while also dramatically lowerin

191 We report buckling of the boundary controlled by the pattern of bo

192 behaviour of the tetrapod is governed by the buckling of the central joint, a mechanical nonlinear mo

193 e swelling mismatch resulted in out-of-plain buckling of the disc gels.

194 If the substrate has a reduced thickness, buckling of the entire structure may also occur.

195 s from differential-growth-driven mechanical buckling of the gut tube as it elongates against the con

196 The localised tearing, shearing and buckling of the Izu-Bonin slab indicates that it remains

197 ng of the M4 inner transmembrane helix and a buckling of the M2 transmembrane helix.

198 ly on damping by deforming two forelimbs and buckling of the proboscis, which also serves to distribu

199 lting actuated form derives from the elastic buckling of the rods subjected to inextensibility.

200 iffness at negative forces attributed to the buckling of the subfragment 2 tail portion.

201 pectroscopy, we directly quantify the atomic buckling of these phases within 0.1- angstrom precision,

202 This buckling of two-dimensional crystals offers a strategy f

203 The tendons of some steering muscles buckle on every wingbeat to accommodate high amplitude m

204 mations inflate bending resistance and delay buckling onset.

205 uid flow irrespective of whether the tube is buckled or not.

206 Previous scleral buckling or pars plana vitrectomy seem to have no impact

207 -standing nematic active sheet that actively buckles out of plane into a centimeter-sized periodic co

208 key intermediates along both the efflux and buckling pathways to pore formation, as seen in the simu

209 By inducing buckling patterns on these films, the correlation betwee

210 t method simulations elucidate the governing buckling phenomena.

211 solids, and confirm that it is essentially a buckling phenomenon.

212 de is a magnetic resonance mode or an oxygen buckling phonon mode.

213 trectomy (PPV) alone versus combined scleral buckling plus PPV (SB+PPV).

214 Scleral buckling plus PPV resulted in greater SOAS outcomes than

215 Scleral buckling plus PPV showed greater SOAS than PPV alone in

216 tomy (PPV), 50% underwent encircling scleral buckling plus PPV, 18.8% underwent repeat PPV, and 6.2%

217 rwent repeat PPV, and 6.2% underwent scleral buckling plus repeat PPV.

218 e (SB) or vitrectomy with or without scleral buckle (PPV+/-SB) between 2013 and 2016.

219 s plana vitrectomy (PPV) or PPV with scleral buckle (PPV-SB).

220 e had a history of high myopia and a scleral buckle procedure for retinal detachment.

221 licone oil tamponade with or without scleral buckling procedure (SBP) for recurrent RD due to PVR.

222 in a water suspension by a swelling-induced buckling process.

223 s of 2D to 3D conversion via a deterministic buckling process.

224 Here, guided mechanical buckling processes provide access to a rich range of com

225 ability is attained by harnessing the unique buckling properties of auxetic elastic materials (buckli

226 M; reflecting bending strength) and cortical buckling ratio (BR; reflecting bone instability) were me

227 es akin to magnetic tweezers contain, in the buckling regime, multiple and branched plectonemes that

228 pological quantum states to sculpt localized buckling regions in the interior of periodic cellular me

229 The salient feature of these localized buckling regions is that they are indistinguishable from

230 ures available in nature that exhibit better buckling resistance are mimicked and modeled by finite e

231 that when a daughter branch is appended, the buckling resistance of a filament changes from linear to

232 gn engineering rods or columns with superior buckling resistance such as in bridges, buildings, and t

233 hine learning designed rods have 150% better buckling resistance than all the rods in the training da

234 wever, falls in the entirely new category of buckling resistance.

235 l that the obtained antimonene polygons have buckled rhombohedral atomic structure, consistent with t

236 Although buckled Sb and Bi honeycombs support 2D topological insu

237 y noncomplex RD repair with either a scleral buckle (SB) or vitrectomy with or without scleral buckle

238 plana vitrectomy (PPV), and combined scleral buckle (SB) plus PPV (SB+PPV).

239 ed with pars plana vitrectomy (PPV), scleral buckle (SB), or PPV plus SB over an 11-year period (Octo

240 tachments (RRDs) can be treated with scleral buckle (SB), pars plana vitrectomy (PPV), or SB combined

241 tly higher success rate with primary scleral buckle (SB; 63%; OR, 2.2; 95% CI, 1.1-4.5) and combined

242 d grade C PVR after primary encircle scleral buckling (SB group - 12 eyes), or pars plana vitrectomy

243 To investigate the effect of scleral buckling (SB) on the morphology and density of human cor

244 ergoing pars plana vitrectomy (PPV), scleral buckling (SB), and combined PPV/SB for primary RRD in 20

245 udies) of pneumatic retinopexy (PR), scleral buckling (SB), pars plana vitrectomy (PPV), and laser pr

246 itrectomy [PPV], laser barricade, or scleral buckle [SB]) were collected.

247 material) and stretchable structures (e.g., buckled shapes, serpentine mesh layouts, kirigami design

248 inition of complex and stimuli-responsive 3D buckled shapes.

249 Scleral buckling sharply declined, and preference for retinal de

250 Paradoxically, such local compressive buckling should not occur given the tensile stresses acr

251 Two-dimensional buckled Si-based silicene has been recently realized by

252 ndicate that MT filaments in a bundle do not buckle simultaneously implying that the applied stress i

253 lt, sliding forces within the midzone cannot buckle spindle microtubules, which allows the cell bound

254 Y rings are just wide enough for the plug to buckle spontaneously in mammalian membranes.

255 ersely, increased detyrosination promoted MT buckling, stiffened the myocyte, and correlated with imp

256 The local buckling strain depends on the relative size of the comp

257 bserved in the yield stress and average post-buckling stress of the CNTs.

258 of bottom-up assembly and simple triaxially buckled structure design.

259 ed metal-ligand fragments form a noncoplanar buckled structure, as a promising structural unit that c

260 results show that after the introduction of buckled structure, improvement in stretchability, toughn

261 izing the direct-bandgap (nearly 5.0 eV), 2D buckled structure.

262 ratio (NPR) behaviors due to the presence of buckled structure.

263 es under tensile strain-low buckled and high buckled structures, which respectively lead to a low and

264 Scleral buckle surgery was performed, but 3 weeks later the pati

265 e of eyes that underwent vitrectomy, scleral buckle surgery, and pneumatic retinopexy were 71.4%, 14.

266 ent after retinoblastoma therapy and scleral buckle surgery.

267 ens from patients subjected to vitrectomy or buckling surgery for RRD.

268 new indenter marker was used during scleral buckling surgery.

269 bited distinct short- and long-period sheath buckling that occurred reversibly out of phase in the ax

270 ereby regulating the compressive forces that buckle the gut tube into loops.

271 ell body, a fraction of meandering Paramecia buckle their body by pushing on the channel walls.

272 The buckling thresholds predicted by the continuum descripti

273 The simulations show that the buckling time strongly and exponentially depends on the

274 o-orders-of-magnitude difference between the buckling times for RNA and DNA revealed by single-molecu

275 es) utilize multi-stable micro-flexures that buckle to perform Boolean computations based purely on m

276 adhesive surfaces, and controlled mechanical buckling to achieve ultralow modulus, highly stretchable

277 out the configurations of the DNA during the buckling transition because they are not directly observ

278 We experimentally observe this buckling transition by stretching and imaging the lamina

279 Mechanical systems, such as buckling transition spring switches, can have engineered

280 DNA under torsional strain undergoes a buckling transition that is the fundamental step in plec

281 ly flat substrate can be forced to undergo a buckling transition(7-9), resulting in a periodically mo

282 e its importance, quantitative models of the buckling transition, in particular to also explain the s

283 ndergoes a hysteretic, temperature-dependent buckling transition.

284 experimentally determined parameters of the buckling transition.

285 nd Brownian dynamics to simulate the DNA/RNA buckling transition.

286 t the observation of first- and second-order buckling transitions between stable mechanical states in

287 ial domain with both minor vein collapse and buckling (turgor loss) of the living cells.

288 tions, methods of planarization of puckered (buckled) two-dimensional systems, modification of crysta

289 constituent, bears load in tension while it buckles under compression.

290 eases, velocity slows, and the lamellipodium buckles upward in a myosin II-independent manner.

291 More extensive segmental buckling was associated with greater increase in AL (P =

292 The enhanced ability of MT bundles to damp buckling waves relative to individual MT filaments, may

293 ral buckle and vitrectomy combined with belt buckle were performed in 4 and 6 eyes, respectively.

294 ential proteoglycan dynamics and inner layer buckling were positively selected during evolution.

295 Filaments buckle when FH1-FH2 is anchored specifically to cover sl

296 Soft, pneumatic actuators that buckle when interior pressure is less than exterior prov

297 Buckling, when the cardiac tube grows between fixed pole

298 the shell can alter mechanical response and buckling, which we show by simulating a model for the nu

299 n individual Ising chain in this material is buckled, with two sites in each unit cell related by a g

300 pe-switching of the silk filament induced by buckling within the droplets.