ライフサイエンスコーパス: bending

1 es them sensitive to mechanical deformation (bending).

2 ering and diffusion to CTxB-induced membrane bending.

3 12-1 seedlings show exaggerated primary root bending.

4 between in-plane elasticity and out-of-plane bending.

5 in the AT-IN arrays due to inward linker DNA bending.

6 newly-discovered mechanism for extreme light-bending.

7 th the surface work function and upward band bending.

8 ition to the previously reported tilting and bending.

9 ed organs leading to differential growth and bending.

10 ssential for damage-specific binding and DNA bending.

11 original efficiency after 5,000 times fully bending.

12 tion between the two factors and induced DNA bending.

13 oxidase 1 showed attenuated hydrotropic root bending.

14 energy offset between major and minor groove bending.

15 rowth between the two sides, leading to root bending.

16 ansport properties that are not sensitive to bending.

17 bility of the flow-diverter with multi-modal bending.

18 ssue strength was measured using three-point bending.

19 ced in an InSb quantum well through external bending.

20 iscosity or molecular crowding upon membrane bending.

21 y nerve activity was recorded during fin ray bending.

22 an RNA structural element that causes axial bending.

23 edges over the same length scale as the band-bending.

24 iochemical wall heterogeneities precede wall bending.

25 can explain the plastic response of cells to bending(4) and quantitatively predict the rate at which

26 Moreover, for concave bending, a significant improvement in detection signal i

27 In response to bending, a strong overpressure is generated in the chann

28 ributed to polarization-induced surface band bending acting as a thermal barrier to electron/hole rec

29 for EHS-1 when FCHO-1 membrane-binding and -bending activity is specifically eliminated in vivo.

30 rks progress toward providing torque without bending actuators.

31 find that the bundle is solid, and stiff to bending, along the long axis, whereas it has a liquid an

32 Bending amplitude did not differ significantly between t

33 Continuum membrane-bending analysis carried out on homology models of mamma

34 erfaces between conventional materials, band bending and alignment are classically controlled by diff

35 levered indicator pin that responds to plate bending and an internal scale to demonstrate changes in

36 nano-flakes enables the absorber conformably bending and attaching to a metal cylinder.

37 tion in uniaxial and biaxial tension, shear, bending and crack propagation, and subsequently demonstr

38 ented tolerance to mechanical stress such as bending and cutting, where it not only does not catastro

39 y modelling the mechanical strains caused by bending and differential growth of the cell wall.

40 integration requires IHF-induced target DNA bending and explain the elusive role of CRISPR leader se

41 taining proteins have been implicated in the bending and fission of TRE, thus regulating endocytic re

42 use of such active metasurfaces for tunable bending and focusing in free-space.

43 tropic proliferation might explain cartilage bending and groove formation at the macro-scale.

44 zigzag HFs, and is required for zigzag hair bending and guard HF cycling.

45 h interhead strain rotates the rings through bending and hinging of the stalk.

46 In addition, we show that membrane bending and ILV formation are directed specifically by t

47 -10 element where they likely facilitate DNA bending and impede transcription bubble collapse.

48 tilized cell shape change linked to folding, bending and invagination of polarized epithelia.

49 ediated endocytosis (CME) involves nanoscale bending and inward budding of the plasma membrane, by wh

50 gnition of the spacer half-site requires DNA bending and leads to full integration.

51 their lipid bilayer membranes, which resist bending and local changes in area, and their cytoskeleto

52 I-2 induced bending and melting of DNA.

53 he pre-initiation steps of promoter binding, bending and melting, and abortive RNA synthesis.

54 egligible strain change up to 180 degrees in bending and over 500% in radial stretching, which is ide

55 ovides insight into how large-scale membrane bending and protein chemistry facilitate lipid permeatio

56 By quantifying the energetics of DNA groove bending and rationalizing the origins of the anisotropy,

57 ning based on DNA deformation, in which both bending and shearing of the nucleosomal DNA are consider

58 opy, we experimentally show the propagation, bending and splitting of slot gap plasmons.

59 sed by considering the mechanisms at play in bending and stretching deformations of atomic monolayers

60 characterizes the relative costs of filament bending and the straining of cohesive bonds between fila

61 signatures and geometrical features, analyze bending and torsion angles, and determine distinct knowl

62 The models reliably capture the filament bending and torsional rigidities and intersubunit torsio

63 yomicroscopy reveal how cofilin enhances the bending and twisting compliance of actin filaments.

64 Bending and twisting deformations can be created under I

65 ond, S3D cofilin only weakly alters filament bending and twisting dynamics and therefore does not int

66 ork model, reveals two types of NCT motions, bending and twisting, with respect to PS1.

67 etween the local deformation of the tissues (bending) and the water pressure in the plant vascular sy

68 adjustments, such as length trimming, shaft bending, and bark stripping [4, 6, 7].

69 used by the increasing severity of stenosis, bending, and branching.

70 s, in which crease folding requires no sheet bending, and random patterns with high-energy folding, i

71 cal signals, including stretch, compression, bending, and shear.

72 precisely integrates activities of sensing, bending, and stabilizing curvature to sculpt membranes w

73 ve multiaxial motions including contraction, bending, and torsion.

74 nteractions, including pressing, stretching, bending, and twisting.

75 distance with the curvilinear distance, the bending angle distribution, and the persistence length.

76 temperature-responsive function at a maximum bending angle of 45 degrees .

77 rchitectures, we have explored the effect of bending aromatic amide beta-sheets using building blocks

78 ) and still experience minimal PCE loss even bending around 180 degrees .

79 r method to investigate the role of membrane bending around the charged voltage sensors of the transi

80 ing microtubules self-organize into parallel bending arrays, guiding varying directions for fast plus

81 sults suggest inherent CTxB-induced membrane bending as a mechanism for initiating CTxB internalizati

82 drive shaft whereas the hook is flexible in bending as a universal joint.

83 nderlying biophysical mechanisms of membrane bending at physiological length scales.

84 These include substrate bending at the duplex-duplex junction and transfer of un

85 Band bending at the TI surface may also lead to coexisting tr

86 hotodetector maintained high stability under bending at various bending radii.

87 loading for (a/w) < 0.3 for the same (a/l); bending begins to play a significant role in failure as

88 fundamental mechanisms that control the self-bending behavior are identified and tested with microsca

89 dual stresses that enable programmable, self-bending behavior.

90 free 5'-terminiin vivo Here we monitored DNA bending by FRET and DNA unpairing using 2-aminopurine ex

91 stigated how these domains contribute to DNA bending by HMGB1 using single-molecule fluorescence reso

92 Our results show that membrane bending by Mic60 is an ancient mechanism, important for

93 tail, but the tail modulates DNA binding and bending by one of the HMG boxes in the FL protein.

94 Fast, continuum membrane-bending calculations reveal a global pattern of charged

95 , emergence of cones, simple and anticlastic bending can be engineered and pre-programmed in a liquid

96 , this article reports the inherent membrane bending capability of cholera toxin subunit B (CTxB) in

97 in protein-free DNA loops suggests that DNA bending causes the modulation in nucleosomes.

98 exhibit highly similar membrane-binding and -bending characteristics in vitro.

99 uctor-like transport behaviors under various bending conditions are detected by scanning tunneling sp

100 ificantly improved cycling performance under bending conditions is achieved.

101 Under bending conditions, the Li-dendrite growth can be furthe

102 pressure monitoring under different, complex bending conditions.

103 only the normal pressure, even under extreme bending conditions.

104 nding potentials are highly localized in the bending coordinate at the transition state.

105 a quantum spin Hall system by control of its bending curvature.

106 channels that varies quadratically with the bending curvature.

107 odel is introduced to quantitatively predict bending curvatures of the fabricated sheets.

108 show excellent fatigue properties during the bending cycle tests.

109 sheet resistance change of <4% after 10 000 bending cycles at a bending radius of 1.0 cm, when suppo

110 The sensor performed within 12% CV after 100 bending cycles demonstrating the robustness of the nanos

111 Devices are mechanically robust for 10,000 bending cycles.

112 ibility, with the nanowires intact up to 500 bending cycles.

113 only a 4% increase in resistance after 4000 bending cycles.

114 ance and unaltered TMR ratio after over 1000 bending cycles.

115 ith negligible performance change after 1000 bending cycles.

116 5%) under substantial stretching (>400%) and bending deformation ( approximately 180 degrees ), which

117 By tuning the volume fraction of the fibers, bending deformation can be controlled.

118 ange their relative alignment to accommodate bending deformation, thus reducing the strain in individ

119 capable of controlling complex twisting and bending deformations simultaneously or separately using

120 terms of the Young's moduli for Hertzian and bending deformations, and the structural damage dependen

121 Interestingly, zigzag hair shaft bending depends on noncanonical NF-kappaB signaling, whi

122 is is achieved herein by using a three-point bending device which is capable of delivering well-defin

123 actors determining the overall preference of bending direction, the dominant contribution is shown to

124 The emission is attributed to band-bending due to the polarization discontinuity at the int

125 ght in the regulation of stem elongation and bending during shade escape.

126 timated by fitting a line to the plot of log bending energy against log variance explained, partial w

127 ical properties of the membrane, such as its bending energy and elasticity, can explain the red-blood

128 ell surface and cortex together with surface bending energy can generate a morphology that satisfies

129 ne bending model, we determined the membrane bending energy for the gel-phase liposomes, and the resu

130 earing energy of nucleosomal DNA outperforms bending energy in nucleosome occupancy prediction and th

131 It is likely due to the anisotropic bending energy of the LC phase of the saturated phosphol

132 t nucleosome dyad positions is attributed to bending energy that is associated with rotational positi

133 s pores directly by reducing the fusion-pore bending energy, and indirectly by concentrating several

134 d incident fluorescence excitation, membrane-bending events are revealed with superresolution.

135 ine the origin of fracture toughness through bending experiments and molecular dynamics (MD) simulati

136 We conducted in situ three-point bending experiments on beams with roughly square cross-s

137 or two binary MGs: Pd82Si18 and Cu46Zr54 The bending experiments show that Pd82Si18 is considerably t

138 o understand the initial stages of nanoscale bending have been limited by experimental resolution.

139 e pairs in a Family A three-way junction and bending in an internal G-U-rich zone.

140 cific DNA sequence, approximately 40% of the bending in the association forms is intrinsic and that a

141 favorable for duplex DNA binding promote DNA bending in the PAM-proximal region during early steps of

142 the PELDOR time traces, and demonstrate that bending, in addition to twist-stretch motions, underpin

143 As membrane bending increases, Sar1 membrane binding is elevated, ul

144 ity of the physisorbed (triplet) O2 and band bending induced by the (O2)(-) radicals.

145 ides in the semi-circle region, to eliminate bending induced mode coupling, and adiabatically tapered

146 Bending-induced asymmetric stresses generate chemical po

147 rite growth can be further aggravated due to bending-induced local plastic deformation and Li-filamen

148 DNA bending is critical for DNA packaging, recognition, and

149 Hypoxic root bending is inhibited by the group VII ethylene response

150 same curvature as in a nucleosome, and that bending is modulating CPD formation.

151 Root bending is preceded by the establishment of an auxin gra

152 ntration along the filopodium independent of bending, lateral shift, or tilting is missing.

153 rly steps, PAM recognition causes severe DNA bending, leading to spontaneous DNA unwinding to form a

154 sliding forces that bend the flagellum, and bending leads to deformations and stresses, which feed b

155 ed the rice (Oryza sativa) LESION AND LAMINA BENDING (LLB) gene that encodes a chloroplast-targeted p

156 sh the fundamental aspects of stretching and bending mechanics of the structure.

157 es into lipid bilayers, supporting an active bending mechanism through wedging.

158 Common molecular mechanisms for bending membranes are evident in different cell biologic

159 mposites were mechanically tested in 4-point bending mode after aging (10,000 thermal cycles).

160 ctuation with over 8% strain at 25 MV m(-1), bending-mode actuation due to asymmetric positioning of

161 By combining these results with a membrane bending model, we determined the membrane bending energy

162 Our smFRET data have revealed distinct bending modes at recombination signal sequence (RSS)-con

163 ion of the IR-active hydrogen stretching and bending modes of NH3 and NH4(+) in aqueous solution, the

164 inear interactions among the first and third bending modes of vibrations of slightly curved beams (ar

165 ults of the coupled effects of torsional and bending modes.

166 ding ones previously shown to alter membrane bending moduli or phase behavior.

167 hat is able to identify rapid changes in the bending modulus and fluidity of vesicle lipid bilayers o

168 two to three orders of magnitude increase in bending modulus compared with conventional polymersomes.

169 and membrane and show that reduction in the bending modulus is directly correlated with parasite inv

170 The bending modulus is found to be 1 kT, which is about two

171 ped vesicle revealed an abrupt change in the bending modulus of the bilayer which could be associated

172 nsion of the red cell and a reduction in the bending modulus of the cell's membrane.

173 bove the rolling cell, suggesting a very low bending modulus of the tether.

174 ext] from 5.1 m to 129 m, corresponding to a bending modulus ranging from 2.2 to 54 (x[Formula: see t

175 decreased bilayer packing, decreased bilayer bending modulus, and increased water penetration.

176 h responses were dominated by sensitivity to bending moment (torque) at the base of the whisker and i

177 rial to polarize in response to a mechanical bending moment and, conversely, to bend in response to a

178 The periodic bending motion of cilia and flagella is thought to arise

179 We find that the continuous bending motion of the Bridge helix (BH) serves as a crit

180 loser during opening, likely through a hinge-bending motion.

181 ate plastic and reversible sinusoidal-shaped bending movements of the neighboring commissural shafts.

182 The initiation of membrane bending occurs at a length scale that is irresolvable by

183 nylon and its anisotropic thermal expansion, bending occurs when a nylon beam is differentially heate

184 ins, a process previously thought to involve bending of an epithelial sheet, but which we now show in

185 artition was observed to be sensitive to the bending of bilayers, indicating that the effect of SP-C

186 indenter-particle physical contact, and the bending of curved elements (beams) modeling the particle

187 lows a flexible protein to stabilize a tight bending of DNA.

188 e distinct TMD conformations, which involves bending of helices VI and VII around flexible glycine hi

189 hroughout a sample which prevents the random bending of light that clouds biological tissues.

190 at the breathing mechanism of 1 involves the bending of metal-ligand bonds and the sliding of interpe

191 lling optical measurement techniques for the bending of micro-mechanical transducers such as cantilev

192 The protein does not induce appreciable bending of nonspecific DNA.

193 " longitudinal pulling causes shortening and bending of platelet-attached fibers, resulting in format

194 s driven by twisting, rotation, buckling and bending of pore walls contributes to the large deformati

195 bases and backbone distortions, with a sharp bending of the duplex accompanied by conformational chan

196 in filaments at [MgATP] </= 0.1 mM and local bending of the filament front upon each myosin head atta

197 otodimerization reaction drives twisting and bending of the individual branches.

198 d stress in one of the layers results in the bending of the linear hybrid structure, thereby minimizi

199 o induce inward (AT-IN) and outward (AT-OUT) bending of the linker DNA.

200 duced porous silicon oxide (PSO) coating and bending of the MC were used as methods of evaluation.

201 olves not only a torsional motion but also a bending of the molecule due to the sp to sp(2) rehybridi

202 ge-scale conformational changes that lead to bending of the nucleic acid helix.

203 sRBD-dsRNA interactions generate only modest bending of the RNA along its helical axis.

204 es in the lower half of the root, triggering bending of the root tip at the elongation zone.

205 s in the transmembrane domain, which include bending of the S6 transmembrane segment and consequent p

206 fish brain drives a basic motor program, the bending of the tail.

207 which effectively tunes the electrical band bending of TiO2 .

208 ral changes are known to involve tilting and bending of various transmembrane helices.

209 investigate the ramifications of target DNA bending on the transposition reaction.

210 Trigger-hair bending or direct application of JA caused a quantal rel

211 at it cannot explain the plastic response to bending or the observed straightening rate.

212 romorph muscles have been largely limited to bending or torsional motions or as tensile actuators wit

213 fic shape changing scenarios, e.g., based on bending, or twisting in prescribed directions, are enabl

214 oncerted trajectories display a strong angle bending oscillation ( approximately 25 degrees oscillati

215 ction in intensity of C-H stretching and C-N bending peaks in infra-red spectrum.

216 pacing relative to the effective (v1, v3, l) bending potentials are highly localized in the bending c

217 impact of this molecular active pump on the bending properties of its lipid environment, we have fun

218 ever, the coupling between CTxB and membrane bending provides an alternate understanding of CTxB-indu

219 exhibiting a TMR ratio as high as 190% under bending radii as small as 5 mm.

220 after wrapping of the flexible sensor, with bending radii down to 5 mm.

221 ined high stability under bending at various bending radii.

222 ange of <4% after 10 000 bending cycles at a bending radius of 1.0 cm, when supported on polyethylene

223 Pressure sensitivity is maintained down to a bending radius of 80 mum.

224 theoretical model relating the experimental bending radius of curvatures of the hydrogels with the Y

225 , including increased deformation, decreased bending resistance, and decreased energy dissipation cap

226 The sensor operates at its bending resonance frequency and has cosine directional c

227 At the bending resonant frequency of the sensors (1.69 kHz) an

228 ling reporter explained the reversed, upward bending response.

229 oresponsive; however, in most cases only the bending responses of these films have been studied, and

230 Removing the bending reverses ion flux and electrical current.

231 the molecule under tension, contour length, bending rigidity and intrinsic stiffness decreased in hy

232 een the physical properties of the membrane (bending rigidity and surface and dipole electrostatic po

233 al case, that spatial variations in membrane bending rigidity associated with lipid domains embedded

234 We quantitatively measure the GO bending rigidity by characterizing the flattening of the

235 e observation that GM1 decreased the bilayer bending rigidity is important for understanding the role

236 about two orders of magnitude lower than the bending rigidity of neat graphene.

237 bility can be smoothed out by increasing the bending rigidity of the coat, allowing for successful bu

238 The bending rigidity of the ER tubule membranes was found to

239 ration technique allowed measurements of the bending rigidity of the fluid phase only, whereas electr

240 ropipette aspiration were used to assess the bending rigidity of the membrane as a function of GM1 co

241 ea compressibility modulus and, as such, the bending rigidity of the membrane is considerably reduced

242 properties, such as membrane undulations and bending rigidity, in a PIP2-dependent manner.

243 crystalline structure, depending on the DNA bending rigidity, which is influenced by the ionic stren

244 To reduce the bending sensitivity, we use composite nanofibres of carb

245 nal double-bended saturation behaviour: both bendings separately follow the standard saturation model

246 ind leg depressor muscles and then stored by bending specialised elements of the thoracic skeleton th

247 magnetic properties under various mechanical bending statuses and show excellent fatigue properties d

248 eased over time, with a 40% reduction in the bending stiffness after 36 h.

249 al-based sensing system (MBSS) with gradient bending stiffness can be designed by connecting gradient

250 a crumpling transition when the microscopic bending stiffness is comparable to kT, the scale of ther

251 esponse to various activating antibodies and bending stiffness of the micropipette.

252 ysical realizations of such membranes have a bending stiffness well in excess of experimentally achie

253 mall RBC patch to compute the shear modulus, bending stiffness, and network parameters, which are sub

254 e that variation in two physical parameters- bending-stiffness of the polypeptide and strength of int

255 We show that bending strain can be used to control the spin orientati

256 This concept of bending strain engineering of spins via topological nano

257 Here the concept of bending strain engineering to tune the spin transport pr

258 arry 25% of the energy of GTP hydrolysis as bending strain, enabling them to drive movement with eff

259 bone width, section modulus (SM; reflecting bending strength) and cortical buckling ratio (BR; refle

260 ower fracture risk because of high BMD, high bending strength, and more stable bones.

261 In the composites, the bending stress is largely dissipated by the scaffolds.

262 nsition from membrane stretching to combined bending, stretching and through-thickness shearing, decr

263 uiding periods and along designed 90 degrees bending structures.

264 nvolves large conformational changes and DNA bending, suggesting how interaction with the cell divisi

265 sion of the ERFVII member HRE2 inhibits root bending, suggesting that primary root growth direction a

266 the aluminas was determined with the 4-point bending test.

267 the spine mechanical properties (two-points bending tests) in a cidaroid (Eucidaris tribuloides) and

268 deflection profile from video recordings of bending tests, (ii) an optimisation algorithm for the ch

269 eater accuracy than previously possible with bending tests, by employing all the available informatio

270 ity and stability during repeated mechanical bending tests.

271 sensor platform was demonstrated with cyclic bending tests.

272 hanical properties that also agree well with bending tests.

273 MBD2 binding to methylated CpGs induces DNA bending that is augmented by the IDR region of the prote

274 sary to facilitate the TM helix breaking and bending that is often needed to satisfy functional imper

275 to facilitate the fragmentation not only by bending the C-F bond of the radical anion out of planari

276 ny degradation to charge storage capacity on bending the electrode.

277 Pulling on both CN and SP levers and bending the emissions curve by 2020 can keep the central

278 rges, thus forming internal electric fields, bending the semiconductor bands, and finally impeding fu

279 asymmetry in hydrodynamic drag or propulsion bending the swimming path into a helix.

280 films with T = 76%) and after 1000 cycles of bending to a 5 mm radius.

281 test and were found insensitive to repeated bending to a small 0.5 cm radius.

282 We used models of whisker bending to quantify mechanical signals (forces and momen

283 Here, the Li-metal anodes are made bending tolerant by integrating Li into bendable scaffol

284 It is anticipated that this bending-tolerant anode can be combined with further elec

285 With the bending-tolerant r-GO/Li-metal anode, bendable lithium-s

286 ersistence lengths were generally larger for bending toward the minor groove, which is thought to ori

287 light-induced motions, including expansion, bending, twisting, and jumping.

288 actively deform, exhibiting at best passive bending under external fields.

289 ntrast, rigid filament bundles slide without bending under motor stress, yielding materials that unde

290 he deformation and stretching vibration, and bending vibration of the OH group of water physisorbed t

291 The intermediate-frequency wagging and bending vibrations have more contribution to electron-ph

292 w only a chaotic pattern and less pronounced bending vibrations.

293 The anisotropy of B-DNA groove bending was quantified for eight DNA sequences by free e

294 hanism is the one that accords best with the bending waveforms of Chlamydomonas flagella.

295 100% retention in charge storage capacity on bending) were observed.

296 , and the weld joint shows high ductility in bending which is accomplished through the operation of m

297 tine GaN(0001) surface exhibited upward band bending, which was partially flattened when exposed to H

298 Ca(2+)-dependent fusion process by membrane bending with a myriad of variations depending on the pro

299 anges of DNA cages drive membrane fusion and bending with predictable outcomes, opening up opportunit

300 yroglutamic acid at the beta2 N terminus and bending within the EGF1 domain.