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1 rgonic reaction, drives the system away from equilibrium.
2 e frozen on returning from nonequilibrium to equilibrium.
3 t was later shown to be forbidden in thermal equilibrium.
4 ot-opaque bodies away from the thermodynamic equilibrium.
5 neighbouring beta-strands shift the Ub/Ub-CR equilibrium.
6 out of the X-Si-CPh plane) contribute to the equilibrium.
7  and pushing replication chemistry away from equilibrium.
8  in a system that is in local but not global equilibrium.
9 mical system to reach a state of statistical equilibrium.
10 o accurately modeling multisolute adsorption equilibrium.
11 uenced by axial chirality and conformational equilibrium.
12 layers hours to reach macroscopic structural equilibrium.
13 ansitions that are not readily accessible in equilibrium.
14  and describe systems far from thermodynamic equilibrium.
15  fast dynamics can drive the whole system to equilibrium.
16 l motion when spectrin filaments are held at equilibrium.
17 acterize the slow dynamics of systems out of equilibrium.
18 quilibrator, in order to reach thermodynamic equilibrium.
19 CBs) is still challenged by slow approach to equilibrium.
20 nd avian evolution, resulting in genome size equilibrium.
21 l and isotopic compositions at thermodynamic equilibrium.
22 at caffeine and 3-CGA concentrations reached equilibrium according to first order kinetics between 6
23  will behave selfishly (by choosing the Nash equilibrium action, namely giving nothing).
24                  Moreover, the monomer-dimer equilibrium affinity constant was determined using nativ
25           All PCBs reached within 95-100% of equilibrium after 56 days of deployment in the system vi
26 imated using multilinear analysis 1 (MA1) or equilibrium analysis (EA).
27 ness, with the same relation holding both in equilibrium and as the system ages.
28  In conclusion, MCL can help maintain immune equilibrium and decrease PGN, S. aureus and MRSA-trigger
29  the catalytic reaction in order to push the equilibrium and enhance the assay fold amplification for
30                                           In equilibrium and kinetic binding experiments [(3)H]RO6957
31 ) by surface plasmon resonance (steady-state equilibrium and kinetic experiments, respectively).
32  multiplatform software named TREND to Track Equilibrium and Nonequilibrium population shifts among t
33 ons have been predicted for a broad range of equilibrium and nonequilibrium systems, but their experi
34  analysis of urea and diethylurea effects on equilibrium and rate constants.
35 ion are dictated by a dynamic conformational equilibrium and that subtle changes in ligand structures
36 he Zn:ligand ratio used, indicating isotopic equilibrium and that the results were not significantly
37 2+) transients, altered intracellular Ca(2+) equilibrium, and caused Vm depolarization.
38                               The dA(*+)/dA* equilibrium, and consequently the reactivity in DNA, is
39 The dynamic range of the RAS was large, with equilibrium angiotensin levels being 8- to 10-fold highe
40 ns of high-performance TE materials, the non-equilibrium approaches offer a fast and controllable fab
41 ted to continue its growth to an oscillating equilibrium around a value of 24% (95% CI: 3-57).
42 ditionally identified the internal acid-base equilibrium as a key determinant of the GCaMP dynamic ra
43 onium salt solutions is explained by a redox equilibrium as shown between oxoammonium salts and trace
44 st MIP was morphologically characterized and equilibrium assays were carried out.
45 y production and failure to reach population equilibrium at the genomic level suggest internal instab
46 ium ions remodel the landscape, shifting the equilibrium away from the extended, partially unfolded s
47                 Here we show that the out-of-equilibrium behavior of a model glass-forming system can
48 s can redistribute in ways not expected from equilibrium behavior.
49 often translates into an equally rich out-of-equilibrium behaviour.
50  the PHn-PHc fragment that indicate it is in equilibrium between "open" and "closed" conformational s
51                                          The equilibrium between (O)S2 and (4)C1 conformations in the
52 The rate of transport is therefore set by an equilibrium between a faster state, where only KIF17 mot
53 PRT) is a hexameric enzyme in conformational equilibrium between an open and seemingly active state a
54                                    A dynamic equilibrium between anchored and diffusive receptors is
55 CO2 near the electrode surface through rapid equilibrium between bicarbonate and dissolved CO2.
56 nd the average size is dictated by a natural equilibrium between bound and unbound CENH3 (and its cha
57  we analyse the data in terms of a two-state equilibrium between compact and extended conformations.
58 e bacterium is challenged to find a delicate equilibrium between expression of MCR-1-mediated colisti
59                             We show that the equilibrium between functional subtypes of sensory neuro
60 thway by which a C-type lectin modulates the equilibrium between infection-driven inflammation and pa
61 formations, but the activated receptor is in equilibrium between multiple conformers that in principl
62                                    A dynamic equilibrium between multiple high- and low-spin species
63 e in temperature, perturbs the thermodynamic equilibrium between native and unfolded states of protei
64 d different K(+) concentrations to shift the equilibrium between nonconductive and conductive states
65                                          The equilibrium between proliferation and quiescence of myog
66               The model accounts for dynamic equilibrium between protein, toxin, and the protein-toxi
67 no acid point mutations on the thermodynamic equilibrium between the folded and unfolded states of a
68 ptake, as well as in maintaining the dynamic equilibrium between the internal and external environmen
69 mational change in which Ub adopts a dynamic equilibrium between the known, common Ub conformation an
70 fully predict point mutations that shift the equilibrium between those two states.
71 ounts of sample, short measurement times and equilibrium binding conditions.
72 th increasing adhesion energy and decreasing equilibrium binding distance.
73 in (L-BH) does not shift this conformational equilibrium, but systematic co-addition of the two resul
74  hold also when the system is brought out-of-equilibrium by a periodic driving.
75 tant involving an R155C substitution the NTD equilibrium can be shifted back to its wild-type positio
76 current density can be attributed to the non-equilibrium carrier transport phenomenon enhanced by the
77 ere surely essential for sustaining far-from-equilibrium chemical dynamics, given their functional re
78 hemical shift differences Deltaomega and the equilibrium chemical shift differences Deltadelta of the
79 otubule cytoskeletal filament - itself a non-equilibrium chemical system.
80 issues, such as the attainment of population equilibrium, compliance with the molecular-clock hypothe
81 iny (NMR-invisible) amount of a deaggregated equilibrium component (presumably monomeric 2) was the r
82                  The extraction kinetics and equilibrium concentrations of caffeine and 3-chlorogenic
83  of strong quantum correlations and far-from-equilibrium conditions can give rise to striking dynamic
84 sts at early time 0-15 ps, likely due to non-equilibrium conditions.
85 many orders of magnitude under thermodynamic equilibrium conditions.
86 roduces oscillations of trypsin under out-of-equilibrium conditions.
87 f matter that emerge under intrinsically non-equilibrium conditions.
88 e consequences of S-glutathionylation on the equilibrium conformational ensemble of BAK1 using all-at
89 y 10 A from the Cd(2+) site affects both the equilibrium constant and the residence time of water, wh
90 e mutant protein retained a highly favorable equilibrium constant for flipping the 1,N(6)-ethenoadeni
91 approximately +28 kcal/mol at 200 degrees C, equilibrium constant K approximately 10(-13)).
92 lack of sensitivity due to high dissociation equilibrium constant KD and non-specificity due to an ab
93 ctrometry is used extensively to measure the equilibrium constant of noncovalent complexes.
94 a substituent parameter and the dimerization equilibrium constant, with para electron-donating substi
95                       However, the estimated equilibrium constants (Keq) for U-V bearing minerals wer
96    The Phax left arrow over right arrow Pheq equilibrium constants at 103 K are 2.21 for 1 and 4.59 f
97                 The rates (kon and koff) and equilibrium constants for both reactions were determined
98 f macromolecular complexes with dissociation equilibrium constants from picomolar to micromolar.
99 rea of calcite, adsorption surface areas and equilibrium constants of clay minerals, and cation excha
100 , we assign an error of 1.1-1.2 log unit for equilibrium constants of several reactions leading to ha
101  free energy and impacting reaction rate and equilibrium constants.
102 V) within a range of potentials after steady equilibrium current of both WEs was established.
103                           The newly reported equilibrium data also allow us to propose rate constant
104 ed thermodynamic stability of each domain by equilibrium denaturation in urea.
105 network therefore remained close to textural equilibrium despite a complex history.
106 allowed us to derive the spectrum of the non-equilibrium (detailed balance broken) statistical system
107 cribed here enables the user to customize an equilibrium dialysis device to fit their own experiments
108 e device was used to successfully measure an equilibrium dissociation constant for Zn(2+) and human s
109                             The low value of equilibrium dissociation constant or affinity unit (KD)
110 rse transacylations, essentially creating an equilibrium distribution of acyl groups.
111 d photoelectron images revealed a highly non-equilibrium distribution of photocarriers in space and e
112 work for how biophysical systems can use non-equilibrium driving to achieve robust function.
113 onal ice crystallites or form because of non-equilibrium dynamical effects.
114 gical constraints can give rise to novel non-equilibrium dynamical patterns that lack any passive cou
115 tor composed of up to 53 qubits to study non-equilibrium dynamics in the transverse-field Ising model
116 dynamic properties of hydration water is its equilibrium dynamics spanning picosecond to nanosecond t
117 rmula: see text] Although finite temperature equilibrium dynamics will not yield hyperuniform states,
118 f the capsid and a complex alteration of its equilibrium dynamics.
119 ng different unbinding energies not only has equilibrium effects on the system, but kinetic effects a
120 shows that W32 oxidation likely involves pre-equilibrium electron transfer followed by proton transfe
121 ge metadynamics simulations to determine the equilibrium ensembles of an insulin molecule under amylo
122 ions utilized generalization of a simplified equilibrium equation.
123 er, we demonstrate that bicarbonate, through equilibrium exchange with dissolved CO2, rather than the
124  strength of the conjugate base such that an equilibrium exists between protonation of the base and p
125 ments testing whether an evolutionary stable equilibrium exists for the three genomic RNAs of Alfalfa
126 DeltaG (double dagger)r disproves that quasi-equilibrium exists in our experiments between protons in
127                                  Kinetic and equilibrium experiments show that poly(dA:dT) tracts per
128 urbations of the monomer/protofibrils pseudo-equilibrium extend to the C-terminal residues in the Abe
129                                 However, non-equilibrium Floquet systems, which are subject to a peri
130 eport that steady states of systems with non-equilibrium fluxes can support topologically protected b
131 and are known to reach a lasting homeostatic equilibrium following a dynamic priming period after bir
132       We characterise such notion of thermal equilibrium for an arbitrary observable via the maximisa
133  or mechanical stress to perturb the folding equilibrium for examining protein stability and the prot
134  activity into a nucleocytoplasmic shuttling equilibrium for visualizing single-cell signaling dynami
135 The three-component reactions proceed by pre-equilibrium formation of a hydrogen-bonded adduct betwee
136  quartet formation, causing the shift of the equilibrium from the hairpin structure to the quadruplex
137  monomeric (Z)-1 that was formed in a mobile equilibrium from the inactive, predominantly dimeric (Z)
138    Using single-component and multicomponent equilibrium gas adsorption measurements, we show that th
139                                    Since non-equilibrium GBs have increased amounts of both strain an
140  a material under irradiation as compared to equilibrium GBs.
141 rity of natural processes occur far from the equilibrium, general theoretical approaches to non-equil
142 ics by the photodetachment of anions with an equilibrium geometry similar to the neutral transition s
143                                          Non-equilibrium hot carriers formed near the interfaces of s
144 exhibited three restoration trajectories: an equilibrium in meadows, a non-linear increase across ste
145 ors controlling the antiparallel-to-parallel equilibrium in muPA.
146  changes in ligand structures can shift this equilibrium in opposite directions, leading to a functio
147 e of the congeners achieved more than 50% of equilibrium in static deployment for the same period.
148 een studied using short-column sedimentation equilibrium in the analytical ultracentrifuge and model-
149 actional loss of PRCs and closer approach to equilibrium in the vibrated deployment resulted in estim
150 thodology is presented here, using Diffusive Equilibrium in Thin-film (DET) gels as high-spatial-reso
151 e unprecedented access to materials far from equilibrium, including high-temperature modifications by
152 ously maintaining chemical systems away from equilibrium, incorporating feedback loops and pushing re
153 el-free cell separation mechanism called non-equilibrium inertial separation array (NISA).
154 describe thermodynamic quantities for out-of-equilibrium interacting many-body systems.
155 ative-like structures; two that appear to be equilibrium intermediates (i.e., populations of new conf
156 s deregulate a subtle dynamic conformational equilibrium involving the N-terminal domain (NTD) with i
157 rce constants of iron bonds, we calculate an equilibrium iron isotope fractionation between silicate
158 estriction of a thermodynamically favourable equilibrium is a common theme in materials processing.
159     Understanding quantum dynamics away from equilibrium is an outstanding challenge in the modern ph
160 anetary atmospheres, as its radiative energy equilibrium is controlled primarily by haze particles in
161 analyses show that the segment ratio at this equilibrium is determined by frequency-dependent selecti
162 tion of opaque bodies, even if thermodynamic equilibrium is not satisfied.
163  then transported to the receiving arm until equilibrium is reached (up to 22 d).
164    While tipping in a fold bifurcation of an equilibrium is well understood, much less is known about
165 jump-walking simulations are able to produce equilibrium isotherms which are typically hidden by the
166               The measurement of a deuterium equilibrium isotope effect (EIE) for the aryl CH...Cl(-)
167 ed to characterize the boronic acid/boronate equilibrium kinetics.
168 ctroscopy method quantifying circulating and equilibrium levels.
169 e pronounced for species of all sizes having equilibrium life history strategy, large species with pe
170 ntrinsic thermal conductivity at the thermal equilibrium limit.
171                                         This equilibrium-limited reaction is favored at a low working
172                        Here we realize a non-equilibrium material characterized by a bandgap whose ed
173                                              Equilibrium measurements between such states enabled the
174 rated with FMP-Red-Dye exhibited depolarized equilibrium membrane potentials compared with GABAAR-nul
175                         We develop a general equilibrium model that encompasses regional variation in
176 rength, and is well described by a two-state equilibrium model.
177 en shown to exist in a dynamic monomer-dimer equilibrium modulated by translocation ligands, and mult
178 te that CNC I, CNC II, CNF I, and CNF II had equilibrium moisture contents of 21.4, 28.6, 33.2, and 3
179 stem offers the possibility of harnessing an equilibrium/nonequilibrium system in tandem with its inh
180  recruitment to the PM and suggest a dynamic equilibrium of Gag-lipid interactions.
181 d as a result of competition in a ring-chain equilibrium of multivalent ureidopyrimidinone monomers a
182                                          The equilibrium of reaction products also shifts to ammonium
183  force that simultaneously explains both the equilibrium of supercooled liquid and the thermal hyster
184  is regulated independently of monomer:dimer equilibrium of the 5'UTR.
185 ata collectively suggest that conformational equilibrium of the A3B active site loops, skewed toward
186 beryllofluoridation alter the conformational equilibrium of the beta3-alpha3 loop close to the phosph
187      We report studies of the conformational equilibrium of this enzyme using small-angle neutron sca
188 esent direct evidence for water dissociation equilibrium on rutile-TiO2(110) by combining supersonic
189 anoscale protein-sensing platform with a non-equilibrium on-off switch that employs dielectrophoretic
190  modes of zetacyt to the bilayers in dynamic equilibrium: one in which zetacyt is peripherally associ
191 to depth changes in the calculated aragonite equilibrium oxygen isotope values implies shallow calcif
192 copy reveals up to a fourfold enhancement in equilibrium oxygen storage capacity under both compressi
193 rving part and detailed balance breaking non-equilibrium part.
194 nt that enables determination of kinetic and equilibrium partition constants.
195       In the water column, PBDEs appeared at equilibrium partitioning between particles and colloids:
196 stochastic evolutionary dynamics along these equilibrium paths.
197 election" operating at every point along the equilibrium paths: stochastic jumps off the paths return
198 g tunnelling microscope tip-assist, a hidden equilibrium phase in a hole-doped bilayer of Sn on Si(11
199              Here we observe and study a non-equilibrium phase transition, the condensation of superm
200 ict and experimentally realize a mixed-order equilibrium phase transition.
201 brium, general theoretical approaches to non-equilibrium phase transitions remain scarce.
202  on a control variable is reminiscent of non-equilibrium phase transitions.
203 dics is uniquely set to study complex out-of-equilibrium phenomena thanks to the simplicity of the un
204        Thereafter, in response to the out-of-equilibrium photocarriers, we observed the spatial redis
205 e strategies that lead to new (quantum Nash) equilibrium points whereby players in some classical gam
206 erved that spatial diffusion increased total equilibrium population abundance in heterogeneous enviro
207   Here, we investigate energy storage in non-equilibrium populations of materials defects, such as th
208 heir size-based, deterministic path to their equilibrium positions, a preset fraction of the flow is
209 rticles with inertial channels with multiple equilibrium positions.
210 es of IK,L were affected by an unstable K(+) equilibrium potential (Veq K(+) ).
211 ents at membrane potentials above the Nernst equilibrium potential for Cl(-) and thus can be used as
212  in proteoliposomes by measuring transporter equilibrium potentials.
213 ases transient stop-flow arm arterial-venous equilibrium pressure and reliably detects responders and
214 ases transient stop-flow arm arterial-venous equilibrium pressure beyond the limits of precision and
215 vely infinite, systems) is compared with the equilibrium probability distribution of the spin overlap
216 ological systems have evolved to harness non-equilibrium processes from the molecular to the macro sc
217  class of observables which exhibits thermal equilibrium properties and we give a recipe to explicitl
218 orithm is revisited and updated to study the equilibrium properties of systems exhibiting quasi-noner
219 of their atomistic structures in relation to equilibrium properties.
220  is much faster (ca. 100 h) and higher K2MX4 equilibrium ratios are obtained (>/=96</=4).
221 ast 20 y on various (bio)molecules, the near-equilibrium regime of oligorotaxanes persists at much hi
222 iple thicknesses of silicone and in situ pre-equilibrium sampling with low density polyethylene (LDPE
223                In the present study, ex situ equilibrium sampling with multiple thicknesses of silico
224 umber of recent highlights, including out-of-equilibrium self-assembly, chemically fuelled molecular
225  to bind the channel when the conformational equilibrium shifts toward the conductive state.
226            Further analysis by sedimentation equilibrium showed that degludec exhibited reversible in
227 irus F protein associate in a monomer-trimer equilibrium (Smith, E.
228 is aided by Pourbaix diagrams, which map the equilibrium solid and solution phases under varying cond
229 s PntAB functions to balance the NADH: NADPH equilibrium specifically in the direction of NADPH.
230 with the concentration of cardiolipin in the equilibrium state (lipid-dependent parameter).
231 tates, which are either able to approach the equilibrium state after deviation from metastability or
232            The pathway and rate to reach the equilibrium state are irrelevant, and the resulting asse
233 aditionally described in terms of the static equilibrium state of Lotka-Volterra equations in which b
234 f key observables such as rate constants and equilibrium state populations to greater precision than
235 ll effect drives the magnon gas into a quasi-equilibrium state that can be described by the Bose-Eins
236 n traditionally focused on the thermodynamic equilibrium state, where one-dimensional assemblies resi
237 le photo-induced chiral spin liquid near the equilibrium state.
238 g the reaction from the initial state to the equilibrium state.
239 model membranes in vitro under thermodynamic equilibrium state.
240 ture at which this orthorhombic phase is the equilibrium state.
241 ses transforms them into highly-excited non- equilibrium states.
242 h concepts from lattice-field theory and non-equilibrium statistical mechanics to introduce a generic
243 flux required to maintain a stable, far-from-equilibrium steady state.
244 ty and time-reversal symmetries in their non-equilibrium steady states.
245 technique Absence of Gradients and Nernstian Equilibrium Stripping (AGNES), 1.7mumolL(-1), amounting
246                                              Equilibrium structural properties of fluid bilayers and
247 ensity functional methods to investigate the equilibrium structure and vibrational frequencies of ext
248  to kinetically trapped (non-dissipative non-equilibrium) structures that heavily depend on the metho
249 its off rate, and dramatically increases its equilibrium surface density.
250                           Bioinspired out-of-equilibrium systems will set the scene for the next gene
251 onstrations of complex and functional out-of-equilibrium systems: cells keep track of time, communica
252 e ultrahot gas giant WASP-121b, which has an equilibrium temperature of approximately 2,500 kelvin.
253             Moreover, the seven planets have equilibrium temperatures low enough to make possible the
254 two S = 1/2 intermediates exist in a dynamic equilibrium that is modulated by the electronic properti
255 the state of the spinal cord as a negotiated equilibrium that reflects the concurrent influences of a
256 r condensation with the amine and tautomeric equilibrium, the corresponding pyrrole-ring unsubstitute
257 izing the system's requirements for reaching equilibrium, the device was used to successfully measure
258 re is expected to be in radiative-conductive equilibrium, the required water vapour would need to be
259 uids had been rejected in the 1970s based on equilibrium-thermodynamic arguments.
260 rusion process can be understood in terms of equilibrium thermodynamics considerations.
261                                     Far-from-equilibrium thermodynamics underpins the emergence of li
262 d dynamic assembly; (4) speculative links to equilibrium thermodynamics.
263                                           At equilibrium, these Mechanically Interlocked Molecules (M
264                                         Near equilibrium, this framework demonstrates a lowered free
265 f circulating immune cells are maintained in equilibrium through signals that enhance the retention o
266 overy and isotope values were independent of equilibrium time and nitrate concentration.
267 e of 50 degrees C, extraction time of 26min, equilibrium time of 29min.
268 ugh the DET gel was determined using varying equilibrium times and nitrate concentrations.
269                    We apply such a notion of equilibrium to a closed quantum system and show that the
270 PCNA sequestration by progerin may shift the equilibrium to favor XPA binding.
271 e mode of action is capable of shifting this equilibrium toward the heme-free apo-sGC species.
272 hift the delicate procoagulant-anticoagulant equilibrium toward thrombosis.
273  Aurora A activating protein TPX2 shifts the equilibrium towards an active T-loop conformation wherea
274 at G0/2 and a split zero-bias anomaly in non-equilibrium transport suggest conduction via spin-polari
275                    Here, we investigated the equilibrium (un)folding intermediate state of T4 phage g
276  of variation production in populations near equilibrium under a balance of constant viability select
277                                        Here, equilibrium unfolding and hydrogen/deuterium exchange mo
278 re, we structurally characterized the stable equilibrium urea unfolding intermediate of V75D at the e
279 tatistically indistinguishable from the true equilibrium values even after a short 7-day deployment.
280                            Maintaining these equilibrium values requires minimal persistent loss or a
281 mical concentrations that deviate from their equilibrium values.
282 Keq 1 > 10(6) M(-1), and the second ion-pair equilibrium was estimated to be Keq 2 = (2.4 +/- 0.4) x
283 nd its mechanical properties and dynamics at equilibrium were analyzed by atomic force microscopy.
284   This causes a transient loss of mechanical equilibrium which facilitates a large cascade of motion.
285 s is the definition of the notion of thermal equilibrium, which can be given as the state that maximi
286 n is the most stable and exists in a dynamic equilibrium with a hybrid i-motif/hairpin species and an
287                       The iron complex is in equilibrium with an N2-free species.
288 -phenylbenzoxazine and the thiols reacted to equilibrium with comparable amounts of reactants and pro
289 herical, cylindrical, worm, or vesicular) in equilibrium with each other.
290 jor catalyst resting states but are in rapid equilibrium with ethylene-opened chelates, (alpha-diimin
291 ulations show that apo-CaM exists in dynamic equilibrium with holo-like conformations, while Ca(2+) u
292 tudies have shown that RNAs exist in dynamic equilibrium with short-lived low-abundance 'excited stat
293 Crick (WC) base pairs (bps) exist in dynamic equilibrium with sparsely populated ( approximately 0.02
294 al force exposure, thioester cleavage was in equilibrium with spontaneous thioester reformation, whic
295  a dithiocarbamate radical that is likely in equilibrium with the corresponding thiuram disulfide dim
296 species communities that engage in a dynamic equilibrium with the host immune system.
297        The skin microbiome exists in dynamic equilibrium with the host, but when the skin is compromi
298 centration of the pi-complex that is both in equilibrium with the mobile pentene phase and in product
299 , Na) dimers that are present in solution in equilibrium with the respective [Co(I)(salophen)M] compl
300 The membrane of an assembling coated pit, in equilibrium with the surrounding plasma membrane, contai

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