ライフサイエンスコーパス: charging

1 came first (11.4 +/- 2.9 s to defibrillator charging).

2 can be dynamically modulated via capacitive charging.

3 energy density should not hinder their fast charging.

4 and reduced at the negative electrode during charging.

5 ntirely independent of Rag guanyl nucleotide charging.

6 e to the regulation of Rag guanyl nucleotide charging.

7 s and of formic acid (FA) for causing higher charging.

8 solved manner, through associated capacitive charging.

9 on period with antitachycardia pacing during charging.

10 is not caused by beam-induced electrostatic charging.

11 e mTORC1 activation without altering Rag GTP charging.

12 from the electrolyte) decompose and form on charging.

13 as the primary gaseous product formed during charging.

14 erials to investigate light-assisted battery charging.

15 uration corresponding to lithium ion battery charging.

16 lizing the reactive bromine generated during charging.

17 chromatography (LC), due to analyte multiple charging.

18 the external dimensions of the anode during charging.

19 g(-1) were obtained after 100 cycles of deep charging (0.005-2 V) at a relatively high current of 100

20 lighting up a warning indicator, sustainably charging a commercial capacitor, and powering a smart wa

21 that oxygen is extracted from the lattice on charging a Li1.2[Ni0.13(2+)Co0.13(3+)Mn0.54(4+)]O2 catho

22 Yet, charging a price to screen out nonusers may screen out p

23 system, which provides enough d.c. power for charging a smart watch or phone battery, is also success

24 During charging, a uniform Mg film was deposited on the electro

25 o for hydrophobic carbon, but is unstable on charging above 3.5 V (in the presence of Li(2)O(2)), oxi

26 It is shown that charging almost always involves ion exchange (swapping o

27 However, charging alone is not sufficient to promote dissociation

28 -tRNA synthetases (ARSs) are responsible for charging amino acids to cognate tRNA molecules, which is

29 In London, congestion-charging and a citywide low-emission zone failed to brin

30 y to the effects of double-layer capacitance charging and adsorbed species in the high scan rate CV.

31 te the influence of radioactivity on surface charging and aggregation kinetics of radioactive particl

32 t that neutral osmolytes may have on surface charging and Coulomb interactions.

33 ve the net effect of reducing the capacitive charging and decreasing the time required to achieve ste

34 h greater pyrolysis temperature due to lower charging and discharging capacities, although the chargi

35 accumulation of lithium hydroxide under both charging and discharging conditions.

36 ctrons more than three times faster than the charging and discharging cycles of surface functional gr

37 ts BPC is a phenomenon balanced by localized charging and discharging events across the membrane.

38 the electrolyte and its functionality during charging and discharging is intricate and involves multi

39 ing and discharging capacities, although the charging and discharging kinetics remain unchanged.

40 ostructured materials seem to exhibit faster charging and discharging kinetics, extended life cycles,

41 During the charging and discharging of lithium-ion-battery cathodes

42 ed entering and exiting CDC nanopores during charging and discharging of the EDLC.

43 in the bulk electrolyte concentration during charging and discharging of the EDLC.

44 nsumption and energy efficiencies during the charging and discharging of the system under several sce

45 uctural changes, and charge flows during the charging and discharging processes for a new high-capaci

46 ociated with its large volume changes during charging and discharging processes, mostly through nanos

47 , by electrochemically switching between the charging and discharging status of battery electrodes th

48 This can be achieved by charging and discharging the electrodes in a controlled

49 more energy, without compromising their fast charging and discharging times.

50 By analyzing the kinetics of Ub charging and discharging, we identified proximal active

51 rn the phase transformations associated with charging and discharging.

52 tween marginal emission rates during battery charging and discharging.

53 ase is found to be dynamically evolving upon charging and discharging.

54 aterials undergo large volume changes during charging and discharging.

55 Additionally, the effect of scan rate on the charging and faradaic currents at these nanoITIES arrays

56 ion that occurs on the iron electrode during charging and idle stand.

57 te amino acid selection, transfer RNA (tRNA) charging and mRNA decoding on the ribosome.

58 ng microscope, thus allowing gate-controlled charging and spectroscopic interrogation of individual t

59 the c expansion range in the early stage of charging and suppressing the structure collapse at high

60 Combining a 33% RES, EVs with controlled charging and unlinking would reduce combined electric- a

61 tography (LC) solvents improves sensitivity, charging, and chromatographic resolution for acidic and

62 What mechanism(s) can explain such high charging, and what is the ultimate limit?

63 magnetically enhanced photon-transport-based charging approach, which enables the dynamic tuning of t

64 lower phase), an aqueous solution of K2MCl4 (charging arm; M = Pt, Pd), and an aqueous solution of ex

65 If one maps this redox capacitive charging as a function of electrode potential one not on

66 widely applicable for investigations of tRNA charging as a parameter in biological regulation.

67 U4 to be a bona fide E2 enzyme through an E2 charging assay.

68 This unique selective charging behavior in different confined porous structure

69 We present a transparent and flexible self-charging biosupercapacitor based on an optimised mediato

70 at phosphoUb has no effect on E1-mediated E2 charging but can affect discharging of E2 enzymes to for

71 pplied, going beyond the traditional view of charging by counter-ion adsorption.

72 ults reveal that the stoichiometry-dependent charging by the support can be used to tune the selectiv

73 on regimes, which shows that the target self-charging can be optimised at a pulse duration of few hun

74 We find that controlled electric vehicle charging can reduce associated generation costs by 23%-3

75 y, demonstrating that defects of alanyl-tRNA charging can result in a wide spectrum of disease manife

76 tial and urgent to endow LIBs with ultrafast charging capability to meet huge demands in the near fut

77 tion of particles because of similar surface charging caused by the decay process.

78 cyclic voltammetry show that supercapacitor charging causes marked changes to the local environments

79 to demonstrate that salt removal between our charging CDI electrodes occurs on a longer time scale th

80 he measured reactivity trends correlate with charging characteristics of a Pt13 cluster on the SiO2 f

81 t-current source for sustainably driving and charging commercial electronics, immediately demonstrati

82 and super-capacitors integrated with a photo-charging component.

83 Adjusting the charging condition leads to long cycle life (over 500 cy

84 of oxygen, which is uniquely possible under charging conditions in a Li-O2 battery.

85 electron transfer kinetics, high background charging current and low current density arising from po

86 The charging current associated with the nanosecond screenin

87 4th to 12th harmonics after quantifying the charging current data using the time-domain response.

88 On the one hand, time dependent decay of the charging current mitigates its impact on the current con

89 Analysis of the decay in the charging current suggests that the desired screening may

90 izes information contained in the background charging current to predict electrode sensitivity to dop

91 e has to be controlled carefully because the charging currents.

92 partial recovery of lithium metal during the charging cycle and a constant accumulation of lithium hy

93 erimental comparisons show that the designed charging cycle can enhance the charging rate, improve th

94 Here, we rationally design a charging cycle to maximize energy-storage efficiency by

95 (SEI) from reduced electrolytes in the first charging cycle.

96 shown to extend the battery lifetime between charging cycles while powering a load.

97 The first voltammetric charging-discharging cycle has an electrode conditioning

98 where non-reversible features during in situ charging-discharging cycles were observed.

99 ctrodes are attractive because of their high charging-discharging speed, long cycle life, low environ

100 ifold advantages of high power density, fast charging-discharging, and long cyclic stability.

101 red in the time domain from constant-current charging/discharging and cyclic voltammetry tests, and f

102 rial that shows high specific capacity, fast charging/discharging capability, and long cycle life for

103 After 17h of charging/discharging cycles a remarkable current enhance

104 tructuring active particles can yield faster charging/discharging kinetics, increased lifespan and re

105 applied, and shows no hysteresis during the charging/discharging processes.

106 ctric capacitors, although presenting faster charging/discharging rates and better stability compared

107 Li x Sn --> Sn --> SnO2 /SnO2-x cycle during charging/discharging.

108 its implications for vehicle efficiency and charging duration and timing.

109 es in an effort to understand supercapacitor charging dynamics.

110 ing, surface reconstructions, contamination, charging effects and surface roughness in single-particl

111 This can be attributed to the removal of charging effects and/or reduced fragmentation, but no ma

112 We believe that the reported charging effects are present for most colloidal nanocrys

113 ch tunability arises from the strong exciton charging effects in monolayer semiconductors, which allo

114 ere offer a convenient approach to probe the charging effects in perovskite solar cells.

115 observation and electrostatic tunability of charging effects in positively charged (X(+)), neutral (

116 At the same time marked layer-dependent charging effects lead to substantial variation in the ap

117 the significance of surface interactions and charging effects requiring new understanding.

118 ng the reversibility of the photoresponse to charging effects.

119 We have verified the improvement in charging efficiency resulting from the use of the alkane

120 , possibly due to particle generation or low charging efficiency.

121 ed systems due to the inherently large donor charging energies ( approximately 45 meV), requiring lar

122 We also find the charging energies for X(+) and X(-) to be nearly identic

123 ice lowers parasitic capacitance, increasing charging energy EC.

124 The trion charging energy is large (30 meV), enhanced by strong co

125 Multiple charging enhances the ion mobility spectrometry separati

126 ral neuropathies, suggesting that these tRNA charging enzymes are uniquely important for the peripher

127 ow that to properly describe and predict the charging equilibrium of viral capsids in general, one ne

128 discover new additives that increase protein charging even further.

129 fficult and leads to voltage polarization on charging, even at modest rates.

130 modifications independently confer high tRNA charging fidelity to the otherwise promiscuous, unmodifi

131 ergoes a temperature dependent shift in tRNA charging fidelity, allowing the enzyme to conditionally

132 In utilizing the sensitivity of this charging fingerprint to redox group environment, one can

133 s patient's return to the operating room and charging for an intervening exam when performing catarac

134 Charging fraction is obtained by counting the fraction o

135 tRNA charging fractions can be measured for individual tRNA s

136 Here, we demonstrate a charging-free TREC consisting of an inexpensive soluble

137 This charging-free TREC system may have potential application

138 By monitoring the capacitor charging frequencies, which are influenced by the concen

139 characterization of the power generation and charging frequency characteristics in glucose analyte ar

140 hium ions required for more power and faster charging generates significant stresses and strains in t

141 y must be reversible on the application of a charging I and V.

142 factors, we find the following: (1) delayed charging (i.e., starting at midnight) leads to higher em

143 t-as they undergo progressive and reversible charging in an electrochemical cell.

144 packs to perform engine cold cranking, slow charging in cold weather, restricted regenerative brakin

145 een implicated in the enhancement of protein charging in ESI) of 14 solution additives on the protein

146 s) with current battery cost, limited public charging infrastructure, and no government subsidy; 2) r

147 A diffusion charging instrument (DiSCMini), that simulates alveolar

148 In completely encapsulated films, negative charging is enhanced leading to uniform optical properti

149 The radioactivity-induced surface charging is highly influenced by several parameters, suc

150 More charging is obtained with the smaller tip sizes for prot

151 of water/methanol/acid, although the average charging is slightly lower owing to contributions of sma

152 cally with methionine engendered at the tRNA charging level occurs in mammalian cells, yeast and arch

153 These low charging levels were validated using acid denaturing gel

154 e state-of-the-art developments in ultrafast charging LIBs by the rational design of materials.

155 ormidable challenges is to develop ultrafast charging LIBs with the rate capability at least one orde

156 cells connected in series for directly photo-charging lithium-ion batteries assembled with a LiFePO4

157 ffer an attractive option for directly photo-charging lithium-ion batteries.

158 ser to the predicted values, suggesting that charging lower than the prediction can be attributed to

159 m the distinct step-by-step photon-transport charging mechanism and the increased latent heat storage

160 We detail on a unique sequential charging mechanism in the hybrid electrode: PTMA undergo

161 >/=9.6 mA, strong enough to be an important charging mechanism of the storm.

162 We introduce a charging mechanism parameter that quantifies the mechani

163 Having elucidated the charging mechanism, we go on to study the factors that a

164 mputer simulations have shown that different charging mechanisms can then operate when a potential is

165 Radioactivity-induced charging mechanisms have been investigated at the micros

166 Furthermore, the charging mechanisms of Li-O2 cells with and without TEMP

167 al studies to give a detailed picture of the charging mechanisms of supercapacitors.

168 Increased understanding and control of charging mechanisms should lead to new strategies for de

169 des direct experimental confirmation of EDLC charging mechanisms that previously were restricted to c

170 lain the factors that control supercapacitor charging mechanisms, and to establish the links between

171 amic measurements of salt concentration in a charging, millimeter-scale CDI system to the results of

172 alculated as increased system emissions from charging minus avoided emissions from discharging.

173 and could be described using a metal-sphere charging model.

174 strate that ion beams, due to their positive charging nature, may be used to observe and test the con

175 It is proposed that surface charging occurs through the adsorption of the imidazoliu

176 rtant skills including reactor construction, charging of a back-pressure regulator, assembly of stain

177 h the oxygen electrode for the photoassisted charging of a lithium-oxygen battery.

178 The charging of a mesoscopic TiO2 layer in a metal halide pe

179 investigated during in-situ electrochemical charging of AB stacked (AB-2LG) and turbostratic (t-2LG)

180 We investigate the electrostatic charging of an agitated bed of identical grains using si

181 fferential resistance is caused by transient charging of an iron phthalocyanine (FePc) molecule on a

182 mponents, an energy loss term related to the charging of appropriately addressable molecular orbitals

183 The latter is triggered by charging of Asp164, the first proton carrier.

184 e of the beads: (i) contact electrification (charging of beads of different materials), (ii) contact

185 re all effective at increasing the extent of charging of deprotonated protein ions in negative ioniza

186 On balance, we find that controlled charging of electric vehicles produces negative net soci

187 hanges in dissipation due to single-electron charging of individual quantum dots in carbon nanotubes.

188 al to a hairpin-turn-like one in response to charging of its ends.

189 etric responses of cations and anions to the charging of nanoconfining surfaces are observed.

190 hat can strongly exceed the gas temperature; charging of nanoparticles through plasma electrons reduc

191 The charging of protein ions formed by nanoelectrospray ioni

192 The effects of electrolyte induced charging of QDs on the performance of QDSSCs have not be

193 d the other arising from the involvement and charging of quantized molecular orbital states.

194 pon mapping the perturbations in interfacial charging of redox elements incorporated into a biologica

195 ly efficient electro-osmosis rooted in space charging of regions with distorted orientation.

196 technique, which exploits the transient self-charging of solid targets irradiated by intense laser pu

197 of implantable medical devices and wireless charging of stationary electric vehicles.

198 tion for removal of the large current due to charging of the electrical double layer as well as surfa

199 Capacitive charging of the electrical double layer at opposing ends

200 potentiostatic condition so that the rate of charging of the film equals the rate of removal of the c

201 The charging of the interface also facilitates anchoring of

202 ble fragmentation that can happen during the charging of the ions or within the first stage of the ma

203 transglutaminase cross-linking and niosomes charging of the protein solution enhanced the gelation p

204 Charging of the well-dissolved alkaline starch suspensio

205 ssociated with increased amino acid flux and charging of tRNAs for branched chain and aromatic amino

206 es ubiquitin-activating enzyme (E1)-mediated charging of Ubc7p with ubiquitin.

207 soline displacement, followed by diversified charging opportunities; 3) government subsidies can be m

208 e type of charge injection, i.e., capacitive charging or ion intercalation, via the choice of the cha

209 to the contribution of the photovoltage, the charging overpotential is greatly reduced.

210 However, the large charging overpotential remains a challenge due to the di

211 e hybridized nanogenerator has a much better charging performance.

212 n was continuous (i.e., it did not require a charging period and did not vary during each step of a c

213 yte and carbon electrode induced by the high charging potential cause the decay of capacity and limit

214 number of ions in the absence of an applied charging potential.

215 rolyte, provides a distinct reduction of the charging potentials by 500 mV.

216 method for quantifying the Fermi levels and charging potentials of free-standing colloidal n-type Zn

217 Here we report a high-efficient self-charging power system for sustainable operation of mobil

218 A flexible self-charging power system is built by integrating a fiber-ba

219 A novel and scalable self-charging power textile is realized by combining yarn sup

220 e in acetonitrile; for positive polarization charging proceeds by exchange of the cations for anions,

221 dered to have significant influence over the charging process and therefore the overall performance o

222 r propose that it is possible to control the charging process resulting in comprehensive enhancements

223 composition into Li, ZrO2, and O2 during the charging process, although the thermodynamic energy of t

224 During the photoassisted charging process, I(-) ions are photoelectrochemically o

225 Computations predict that during the charging process, the oxygen ion near the Li vacancy is

226 two-phase coexistence throughout the entire charging process.

227 considerably lower overpotential during the charging process.

228 ay governs the morphology of the discharging/charging products in Li-O2 cells.

229 nt density of 0.1 mA/cm(2) with a consistent charging profile, good capacity retention, and O(2) dete

230 functions of many of these upregulated tRNA charging proteins may together promote WS disease pathog

231 states than the theoretical maximum protein charging protonation limit in ESI that is predicted on t

232 de minimal direct GHG reductions, controlled charging provides load flexibility, lowering the cost of

233 ed redox group contributes to an interfacial charging (quantifiable by redox capacitance) that can be

234 On charging, quantitative LiOH oxidation occurs at 3.1 V, w

235 , the optical charging strategy improves the charging rate by more than 270% and triples the amount o

236 50% of the capacitance is retained when the charging rate increases from 10 to 10,000 mV/s.

237 ence time, and pollutant emissions, when the charging rate or composition of any waste is varying.

238 the designed charging cycle can enhance the charging rate, improve the maximum energy-storage effici

239 llers to improve the thermal-diffusion-based charging rate, which often leads to limited enhancement

240 The opposite holds for lower charging rates of poor wastes (biodegradables, biosludge

241 Lower charging rates of rich wastes (plastics, paper, etc.) or

242 ge materials, to simultaneously achieve fast charging rates, large phase-change enthalpy, and high so

243 excellent Li-ion capacity at extremely high charging rates.

244 stabilization mechanisms as well as surface charging scenarios in reactive and nonreactive porous me

245 n the northern Midwest regardless of assumed charging scheme and marginal emissions estimation method

246 city demand under controlled vs uncontrolled charging schemes.

247 y emission factors, regional boundaries, and charging schemes.

248 recognition elements (here antibodies), this charging signal is able to sensitively transduce the rec

249 om the mean CO2 emissions factor for a given charging site among both marginal and average emissions

250 nce these organic batteries are excelling in charging speed and cycling stability.

251 which often leads to limited enhancement of charging speed and sacrificed energy storage capacity.

252 This binding is independent of the charging state of tRNA but is regulated by the redox sta

253 ic-vehicle charging using 10 methods at nine charging station locations around the United States.

254 analysis presented here directly couple the charging status of bound biomolecules to readout of liqu

255 Besides, this charging step results in complex phase transformations t

256 This charging strategy and understanding of the reactions in

257 h conventional thermal charging, the optical charging strategy improves the charging rate by more tha

258 lized unless lithium-ion batteries with self-charging suppliers will be developed.

259 on application of a potential supercapacitor charging takes place by adsorption of counterions and de

260 substantial potential-dependent interfacial charging that can be sensitively probed and frequency-re

261 al membrane, exhibit constitutive [(32)P]GTP charging that is unaltered by amino acid withdrawal.

262 The 'charging' (that is, ENSO imprinting the North Tropical A

263 However, charging the cross-linked protein solution with niosomal

264 t that currents applied during deionization (charging the EDL) will be different from those used in r

265 t time that up to 83% of the energy used for charging the electrodes during desalination can be recov

266 fficient than its cytoplasmic counterpart in charging the mitochondrial tRNA(Gly) isoacceptor, which

267 Upon charging the molecule in a gated junction, we found repr

268 Charging the supercapacitor electrodes initiates the spo

269 "Charging" the second type of particles with NO was reali

270 With a single YOYO-1 charging, the column can be used for more than 40 runs,

271 Compared with conventional thermal charging, the optical charging strategy improves the cha

272 During charging, the oxidation reaction at significantly reduce

273 size-dependent interplay of the metal domain charging, the relative band-alignments, and the resultin

274 O3 (-) indicates that LiOH can be removed on charging; the electrodes do not clog, even after multipl

275 detectable signal varies in relation to the charging time and resistive and capacitive noise.

276 relatively weakly coupled systems within the charging time constant.

277 ms, the scan rate corresponding to nanoscale charging time constants appears to be suitable for the u

278 track phase transformation as a function of charging time in individual lithium iron phosphate batte

279 s effectively deconvolutes the effect of the charging time on the observed frequency response.

280 Transducer adaptation and membrane-charging time produced bandpass filtering of the recepto

281 s on a longer time scale than the capacitive charging time scales of our CDI cell.

282 a discrete-time feedback loop that equalizes charging time, digitize temperature directly.

283 The short charging times and high power capabilities associated wi

284 anion diffusion and intercalation, affording charging times of around one minute with a current densi

285 Charging times of seconds to minutes, with power densiti

286 Oxidation of Li(2)CO(3) on charging to approximately 4 V is incomplete; Li(2)CO(3)

287 odel that defines conditions for exponential charging to occur and provides insights into the mechani

288 On charging, TTF is oxidized to TTF(+) at the cathode surfa

289 On charging under illumination, triiodide ions are generate

290 This self-charging unit can be universally applied as a standard '

291 ting EV adoption with adoption of controlled charging, unlinked fuel economy regulations, and renewab

292 ons factors associated with electric-vehicle charging using 10 methods at nine charging station locat

293 ed and demonstrated to correlate the maximum charging voltage of a supercapacitor with the capacitive

294 The charging voltage reduction translates to energy savings

295 Beyond the maximum charging voltage, a supercapacitor may still operate, bu

296 e apparent lack of dendrite formation during charging which is one of the crucial concerns of using a

297 stems still require external electricity for charging, which complicates system designs and limits th

298 increased upper cutoff voltage (UCV) during charging, which delivers significantly increased specifi

299 We simulate charging with a discrete-element model including electri

300 The increased charging with the smaller tip sizes for proteins with a