ライフサイエンスコーパス: coulombic

1 igh fluorophilicity of [2]+ arises from both Coulombic and cooperative effects which lead to formatio

2 eracts with other molecules through screened Coulombic and double-layer forces.

3 values, obtained from a novel separation of coulombic and Hofmeister effects.

4 er structures in the gas phase due to strong Coulombic and hydrogen-bonding interactions.

5 icult to isolate effects such as the role of Coulombic and hydrogen-bonding interactions.

6 Moreover, we find that Coulombic and intrinsic contributions to membrane bindin

7 eld in conjunction with ReaxFF and including Coulombic and Lennard-Jones interactions is employed to

8 cking effects, which can be partitioned into Coulombic and overlap effects.

9 ts (epsilon(eff) and epsilon(p)) required in Coulombic and Poisson-Boltzmann models.

10 nergy of the binding and its two components, Coulombic and reaction field energy.

11 Standard implementations of coulombic and solvation effects are seen to be less impo

12 Coulombic and van der Waals energy components determined

13 reveal strong intermolecular van der Waals, Coulombic, and H-bond interactions in striking agreement

14 ely; however, large losses in van der Waals, Coulombic, and H-bond interactions strongly suggest that

15 force field that includes hydrogen bonding, Coulombic, and hydrophobic terms, was used to model the

16 olenses were prepared from the particles via Coulombic assembly onto a silane-modified glass substrat

17 holes, which can more easily overcome their coulombic attraction and form free charges.

18 -binding is a competition between the strong coulombic attraction and the large cost of desolvating t

19 s, and an enthalpic component, stemming from Coulombic attraction between opposite charges.

20 o nanoelectrospray ionization as a result of Coulombic attraction between positively charged protein

21 Second, Coulombic attraction between the separated charges favor

22 parated radical ion pair is a consequence of Coulombic attraction in the contact radical ion pair and

23 ognition process, which relies on an initial Coulombic attraction of anionic SAMs to the cationic HBS

24 is uncharged and thereby lacks the intrinsic Coulombic attraction of the phosphinate anion to the act

25 inhibited by supramolecular factors such as Coulombic attraction or repulsion between a charged gues

26 t the cytoplasmic end of TM2, is caused by a Coulombic attraction to E465, at the cytoplasmic end of

27 fs (tryptophan zipper, disulfide, d-Pro-Gly, Coulombic attraction, l-Pro-Gly) enhance formation rates

28 to membranes are determined by a long-range Coulombic attraction, the hydrophobic effect, and a shor

29 han would be expected on the basis of simple Coulombic attraction.

30 cular, strong correlations are found between Coulombic attractions and the electrostatic desolvation

31 can provide conformational stabilization via Coulombic attractions that do not require entropically c

32 e LUMO, and hence lowers Ueff, the effective Coulombic barrier to charge transfer.

33 s (I37K, Q40K, and V38E) lead to significant Coulombic changes that weaken favorable van der Waals in

34 sition 63 (N) at the middle of the IC1 and a Coulombic charge interaction between the positive charge

35 on potentials (alpha-values) quantifying non-Coulombic chemical interactions of KGlu with unit area o

36 At the same time, the Coulombic component of the binding energy was found to f

37 The non-coulombic contribution to the free energy of global wrap

38 ential at the polyion surface, we obtain the coulombic contribution to the salt-polyelectrolyte prefe

39 The binding is dominated by the coulombic contributions, which account for why the toxin

40 he conductivity to a decrease in the on-site Coulombic correlation energy (U), as the dimers form a s

41 This intermolecular Coulombic decay (ICD) process has since been shown to be

42 and charge transfer, such as intermolecular Coulombic decay and electron-transfer mediated decay (ET

43 A well-known example is interatomic Coulombic decay, where an excited atom relaxes by transf

44 -) largely compensates for the destabilizing Coulombic effect of any salt on the binding of this asse

45 FrdA E49Q and SdhA Q50E mutants suggest that coulombic effects and the electronic state of the FAD ar

46 ind guests in solution; cavity enclosure and coulombic effects appear to be crucial drivers of host-g

47 peration conditions which would minimize the Coulombic effects are discussed.

48 cts between hemes bL and bH and intermonomer Coulombic effects between bL hemes.

49 it was necessary to incorporate intramonomer Coulombic effects between hemes bL and bH and intermonom

50 However, large ion populations may manifest Coulombic effects contributing to the spatial dispersion

51 In this study, we present an analysis of Coulombic effects on IMS resolution.

52 ntermediate comes from studies of steric and Coulombic effects on the quenching rate constants and fr

53 Owing to favorable Coulombic effects, the para-derivative [1]+ has a very h

54 cycles indicates excellent reversibility and coulombic efficiencies above 99%.

55 volumetric energy and power density values, coulombic efficiencies in excess of 95%, and stability o

56 with capacities of nearly 900 mA h g(-1) and Coulombic efficiencies in excess of 99%.

57 s with remarkable cycling stability and high coulombic efficiencies in excess of 99.5%.

58 Li-SPAN cells cycle trouble free and at high Coulombic efficiencies in simple carbonate electrolytes.

59 Coulombic efficiencies near 100 % for every cycle, sugge

60 se nanoparticles to achieve high first-cycle Coulombic efficiencies of 94% to >100%.

61 capacity decay, low rate capacities and low Coulombic efficiencies.

62 mA g(-1), with only 11% capacity fade and a Coulombic efficiency >99%.

63 g(-1) at 100 mA g(-1) after 50 cycles), high coulombic efficiency (>95%), excellent cycling stability

64 lithium deposition and significantly improve Coulombic efficiency (99% over 400 cycles at a current d

65 fter 200 cycles at 0.2C), and a high average Coulombic efficiency (99.7% from the second cycle to the

66 -electrolyte contact area, resulting in high Coulombic efficiency (99.87%) and volumetric capacity (1

67 rnately catalyzing anodic acetate oxidation (Coulombic efficiency (CE) 85.3%) and cathodic denitrific

68 t 9.35 +/- 0.28 g Fe3O4-Fe/L, resulting in a Coulombic efficiency (CE) for iron oxidation of 93.5 +/-

69 Consequently, the Coulombic efficiency (CE) increased: 57% for 0.02 g of F

70 anode materials to achieve high first cycle Coulombic efficiency (CE) of >100% or serve as an excell

71 over a period of 12 weeks and had an average Coulombic efficiency (CE) of 84.1 +/- 1.1% at practicall

72 Mg electrodeposition was achieved with high Coulombic efficiency (CE) of 90% and high current densit

73 only 10 mM bicarbonate buffer and an average Coulombic Efficiency (CE) of 93%.

74 Coulombic efficiency (CE) varied by electron donor, with

75 Furthermore, the measured Coulombic efficiency (CE) was at least 79%, which is 2.5

76 ate cycling of a lithium metal anode at high Coulombic efficiency (up to 99.1%) without dendrite grow

77 cled at 450 degrees Celsius with 98 per cent Coulombic efficiency and 73 per cent round-trip energy e

78 gh energy and power performance, nearly 100% coulombic efficiency and 85% energy efficiency after 25,

79 /- 4.35%, while the average percent error of Coulombic efficiency and COD removal rate predictions we

80 /Li2 O interface are critical to enhance the coulombic efficiency and cyclic performance of SnO2 -bas

81 nt species of VFA by using two methods i.e., coulombic efficiency and cyclic voltammetry was investig

82 60 mA h g(-1)) and lowest potential, but low Coulombic efficiency and formation of lithium dendrites

83 f lithium metal anodes suffers from the poor Coulombic efficiency and growth of lithium dendrites.

84 ransport towards the Li-metal, also has high Coulombic efficiency and kept 93 % of its capacity after

85 to achieve high sulfur utilization with high Coulombic efficiency and long cycle life of Li-S batteri

86 hiation-induced strain and thus exhibit high Coulombic efficiency and long cycle life.

87 polymer/LLZT-2LiF/LiFePO4 battery has a high Coulombic efficiency and long cycle life; a Li-S cell wi

88 modified electrode achieved greatly enhanced Coulombic efficiency and longer cycle life.

89 ing lithium plating/stripping results in low Coulombic efficiency and severe safety hazards.

90 h the supramolecular capsules retains a high Coulombic efficiency and shows a large increase in capac

91 capacity of approximately 110 mAh g(-1) with Coulombic efficiency approximately 98%, at a current den

92 60 mAh g(-1) at 6 C, over 6,000 cycles with Coulombic efficiency approximately 99%.

93 A low operational voltage and high coulombic efficiency are achieved by using a novel compo

94 However, low first-cycle Coulombic efficiency as a result of the formation of a s

95 over the MCMB reference but present a lower Coulombic efficiency as well as a higher capacity loss p

96 to cycle up to 1000 times, with nearly 100% coulombic efficiency at both low (0.15 coulomb) and high

97 unmodified samples, which usually show rapid Coulombic efficiency decay in fewer than 100 cycles.

98 but suffer from rapid capacity fade and low Coulombic efficiency due to the high permeability of red

99 , leading to serious safety concerns and low Coulombic efficiency during charge/discharge cycles.

100 However, dendrite growth and limited Coulombic efficiency during cycling have prevented its p

101 86% incommensurate sample achieves above 99% coulombic efficiency exhibiting 930 mAh g(-1) specific c

102 of approximately 1400 mA h g(-1) with a low Coulombic efficiency for the first cycle (approximately

103 The Coulombic efficiency improves to approximately 99% for m

104 for over 250 cycles, and outstanding average Coulombic efficiency in excess of 99.9%.

105 ted here will be generally useful to enhance Coulombic efficiency in many electrochemical systems (e.

106 Reduced coulombic efficiency is observed at low rates (<25 mVs(-

107 resulted in similar organic removal, but the Coulombic efficiency obtained from the MPPC was 21 times

108 The use of fluoromethane shows a high coulombic efficiency of 97% for cycling lithium metal a

109 ile showing excellent long-term performance (coulombic efficiency of 100 % and energy efficiency of 7

110 chieve over 260 mAh/g after 700 cycles and a Coulombic efficiency of 101.1%, without the use of harmf

111 Besides, a maximum coulombic efficiency of 26.87% with 91% COD removal was

112 er squared (mA cm(-2)) of applied current at coulombic efficiency of 35% (35% of the applied current

113 pacity as high as 301 mAh g(-1) with initial Coulombic efficiency of 93.2%.

114 fic capacity of 1,030 mAh g(-1) at 0.5 C and Coulombic efficiency of 98.4% over 1,000 cycles are achi

115 ) for more than 1,000 cycles with an average Coulombic efficiency of 98.4%.

116 ay as low as 0.046% per cycle and an average coulombic efficiency of 98.5% was achieved.

117 close to 600 mAh g(-1) at a high rate with a Coulombic efficiency of 99 over 160 cycles, an extremely

118 raphene and stability over 100 cycles with a Coulombic efficiency of 99.3% at a current rate of 0.2 C

119 state Li/LiFePO4 cells showed a notably high Coulombic efficiency of 99.8-100% over 640 cycles.

120 te to the electrode leading to not only high coulombic efficiency of 99.9% but also maintaining high

121 ity of 802 mAh g(-1) after 659 cycles with a Coulombic efficiency of 99.9%, which outperforms convent

122 performance is enabled by a stable half-cell coulombic efficiency of 99.97%, averaged over the first

123 ecific capacity of about 70 mA h g(-1) and a Coulombic efficiency of approximately 98 per cent.

124 apacity of approximately 100 mAh g(-1) and a Coulombic efficiency of approximately 99% over hundreds

125 duction rate of 49.9 mmol/day . m(2), with a Coulombic efficiency of over 90%.

126 t inserting sulfur into pores of carbon, the coulombic efficiency of SC/Li cell in the new DOL/D2 ele

127 lexes, plays a significant role in enhancing coulombic efficiency of the corresponding solvated Mg co

128 to improvements in the voltage stability and coulombic efficiency of the electrolyte.

129 High coulombic efficiency of up to 94 % was achieved in dimet

130 ectrolyte showed good cyclability and a high coulombic efficiency over 40 charge/discharge cycles.

131 ng up to 99% of their capacity and 99 +/- 1% Coulombic efficiency over 50 cycles by bulk electrolysis

132 ire arrays reaches 969.72 mAh . g(-1) with a coulombic efficiency over 99% at 500 mA . g(-1) after 50

133 The anode Coulombic efficiency was 44-69%, which is comparable to

134 Thus, the Coulombic efficiency was approximately 16% higher in the

135 A bioanode with high current density and coulombic efficiency was developed by co-immobilization

136 d Mg metal allows reversible operation (100% Coulombic efficiency) with no dendrite formation.

137 5 g L(-1) acetate) at 379 g m(-2) d(-1) (36% Coulombic efficiency).

138 cific capacity of 1,540 mAh g(-1) with a 75% coulombic efficiency, and an 86% incommensurate sample a

139 res of the solid electrolyte interphase, low Coulombic efficiency, and dendritic growth of Li.

140 ock to achieve high sulfur utilization, high Coulombic efficiency, and long cycle life.

141 by issues related to dendrite growth and low Coulombic efficiency, CE.

142 ic charge/discharge capacities and excellent Coulombic efficiency, demonstrating the effectiveness of

143 near the surface, which leads to a decreased coulombic efficiency, likely because of trapped Li withi

144 new electrolyte demonstrates a close to 100% coulombic efficiency, no dendrite formation, and stable

145 be the optimized parameter toward capacity, Coulombic efficiency, stability, and rate capability enh

146 Organic loading in a fed-batch MFC affected Coulombic efficiency, which decreased from 40% at 0.66 g

147 uel cells with increased current density and coulombic efficiency.

148 methane microbial fuel cell operates at high Coulombic efficiency.

149 exhibits a good cycle life and an excellent coulombic efficiency.

150 from the growth of lithium dendrites and low Coulombic efficiency.

151 ass) for >1,000 cycles at approximately 100% coulombic efficiency.

152 Ah g(-1) reversible capacity and nearly 100% Coulombic efficiency.

153 ng with excellent cycling stability and high coulombic efficiency.

154 in terms of capacity, cycling stability, and Coulombic efficiency.

155 rbide particles cycle lithium-ions with high Coulombic efficiency.

156 based batteries, cause safety issues and low Coulombic efficiency.

157 r approximately 30 h with approximately 100% Coulombic efficiency.

158 ds the leading end toward the anode, because Coulombic (electrophoretic) forces are dominant on negat

159 )obs) by way of an analytic treatment of the Coulombic end effect (CEE).

160 model indicates that the axial range of the Coulombic end effect for ss DNA extends over approximate

161 We quantify Coulombic end effects (CEE) on oligocation-nucleic acid

162 Coulombic end effects must be considered when oligonucle

163 g a simple two-state thermodynamic model for Coulombic end effects, which accounts for our finding th

164 relation of DeltaH and DeltaS parameters and Coulombic energies of the various configurations of the

165 the correlation include the change in total Coulombic energy and solvent-accessible surface area.

166 ucleus-independent chemical shift (NICS) and Coulombic energy of 15 j,k-fulvalenes (j, k = 3, 5, 7, 9

167 eceptor uses surface area, total energy, and Coulombic energy to achieve affinity.

168 e in the 2-4 mum size range and then undergo Coulombic fission.

169 interplay between the long-range attractive Coulombic force, the short-range repulsive force and the

170 ttraction overlaid with a normally repulsive Coulombic force.

171 We find that long-range Coulombic forces associated with the highly charged nucl

172 ller in PTH2 than PTH1) as well as repulsive Coulombic forces between amino acids of like-charge (a p

173 RNase A, and illuminate the general role of Coulombic forces between proteins and nucleic acids.

174 If the anion is mobile, Coulombic forces hold this species in close proximity to

175 polar molecules can be driven by fluctuating Coulombic forces induced by flowing polar liquids at nan

176 Thus, Coulombic forces mediate extracellular and intracellular

177 ed and understood in terms of intramolecular Coulombic forces.

178 and were analyzed in terms of the resulting Coulombic forces.

179 ed conformation in dimethyl sulfoxide due to Coulombic forces.

180 K(obs) and on Delta H degrees (obs) dissects coulombic, Hofmeister, and osmotic contributions to thes

181 the tested solutes on ProP appear to be non-coulombic in nature.

182 cling conditions, as well as the first-cycle coulombic inefficiency.

183 Here, the substituent effect is a Coulombic interaction (field effect) of the distributed

184 ction of an attractive side-chain/side-chain Coulombic interaction at the chain termini further stabi

185 nt on salt concentration, as expected from a coulombic interaction between a cationic side chain and

186 substitution, designed to create a favorable Coulombic interaction between ONC and a phosphoryl group

187 inally, evidence is presented that shows the Coulombic interaction between the charged analyte and cl

188 A simple, empirical model based on the Coulombic interaction between the intercalated cation an

189 In the case of HP7, the Coulombic interaction between the terminal NH3(+) and CO

190 This Coulombic interaction can be used to optimize selectivit

191 hange at the chain termini implies that this Coulombic interaction contributes before or at the trans

192 hat this potentially attractive interhelical Coulombic interaction has little or no influence on heli

193 At high ionic strengths the Coulombic interaction is effectively shielded, leading t

194 ent of this catalysis boosting effect to the Coulombic interaction of these positive charges with the

195 Coulombic interaction strongly favors the open conformat

196 pole-dipole coupling, referred to as a super-Coulombic interaction, is a result of an effective inter

197 with two chain ends in close contact through Coulombic interaction.

198 fts in our studies indicates that additional Coulombic interactions across the nonspecific-binding in

199 ent that aligns the patches that would favor Coulombic interactions along the chain.

200 ivity reflects screening of weak, repulsive, Coulombic interactions among charges separated by more t

201 cid-Ke-Base-Eg, suggesting that interhelical Coulombic interactions and a buried polar interaction ar

202 minates between guanine and adenine by using Coulombic interactions and a network of hydrogen bonds.

203 n, with no limitations due to intermolecular Coulombic interactions and nonspecific binding.

204 gh an initial Rayleigh instability driven by Coulombic interactions and show how the intermediate sta

205 ernst-Planck (PNP2) theory to compute (mean) Coulombic interactions and thus to examine the role of t

206 ether these data demonstrate that long-range Coulombic interactions are an important feature in catal

207 -Base-a1 heterodimer, potentially attractive Coulombic interactions are expected in both orientations

208 ing in the native protein, and the favorable Coulombic interactions are reduced at low ionic strength

209 This implies that Coulombic interactions are weak, or that attractive and

210 reversing loop and the addition of favorable Coulombic interactions at the sequence termini.

211 ew tool has been used to explore the role of Coulombic interactions between a core position on one he

212 Still, nonspecific Coulombic interactions between cationic molecules and an

213 volves a very large number (>/similar 20) of coulombic interactions between DNA phosphates and positi

214 he electrostatic energy as a sum of pairwise Coulombic interactions between effective fixed atomic ch

215 esigned and synthesised peptides to show how Coulombic interactions between ionizable 2,3-diaminoprop

216 nts and RO, and that TS exhibits most of the Coulombic interactions between R and O.

217 Interhelical Coulombic interactions between residues at the e and g p

218 ost-guest interactions to overcome repulsive Coulombic interactions between the cationic M12L24 cages

219 smectic-ordered ionic liquid crystal through Coulombic interactions between the ion species.

220 Coulombic interactions between the P0 and P2 subsites an

221 such that exclusively favorable interhelical Coulombic interactions can occur only in the parallel or

222 We conclude that Coulombic interactions cause an oligocation (with ZL < |

223 ndence of the solvation energy; screening of Coulombic interactions contributes only in a minor way.

224 n the antiparallel orientation, interhelical Coulombic interactions favor the parallel orientation an

225 To determine the energetic consequences of Coulombic interactions for helix orientation preference,

226 an provide valuable insight into the role of Coulombic interactions in enzymatic catalysis.

227 rged microspheres because of their repulsive Coulombic interactions in solution.

228 Coulombic interactions in the global wrap must involve b

229 eraction enthalpy is the relief of repulsive Coulombic interactions in the unbound state.

230 bition indicates that nearly eight favorable Coulombic interactions occur in the RNase A.OVS complex.

231 t in major grooves of O pre-TS, forming most Coulombic interactions of RO and burying aromatic carbon

232 Stabilizing Coulombic interactions of this sort are found with many

233 Long-range Coulombic interactions on the surfaces of proteins are w

234 It was found that the Z-scores of Coulombic interactions peak at a considerably negative v

235 sole nucleating event; it also suggests that Coulombic interactions should be considered in the desig

236 His85 reflects mainly effects of long-range Coulombic interactions that are screenable by salt.

237 e a detailed picture of the contributions of Coulombic interactions to binding and catalysis by RNase

238 utility, as it reflects the contribution of Coulombic interactions to the uniform binding of the bou

239 As one would anticipate, Coulombic interactions under the periodic boundary condi

240 g, though small, are viewed as signatures of Coulombic interactions which support theories of polyele

241 phosphate is positioned to form medium-range Coulombic interactions with Lys 66.

242 shoe-shaped structure to engender long-range Coulombic interactions with RNase 1, which is cationic.

243 the solvent available to form complementary Coulombic interactions with the polar residues of the pr

244 nsfer process that is strongly influenced by Coulombic interactions with the proximal cubane cluster

245 olecule are ideally suited to forming strong Coulombic interactions with two contiguous phosphate gro

246 All these findings indicate that the Coulombic interactions within WT protein-protein complex

247 Waals interactions, (2) increased favorable Coulombic interactions, and (3) decreased unfavorable to

248 This facilitated diffusion is mediated by Coulombic interactions, as the extent is diminished by t

249 These factors include Coulombic interactions, hydrogen bonding, and solvation,

250 intermediate complex, which is stabilized by Coulombic interactions, prior to the formation of a Mich

251 fferences are largely determined by internal Coulombic interactions.

252 ly damp the possible periodic distortions in Coulombic interactions.

253 ectrostatic potentials results in disfavored Coulombic interactions.

254 m ionic screening of unfavorable short-range Coulombic interactions.

255 hosphoryl groups in the RNA backbone through Coulombic interactions.

256 e of unfavorable self-energies and repulsive Coulombic interactions.

257 fer rates, are conventionally limited to the Coulombic near-field.

258 es is driven thermodynamically by attractive Coulombic occlusion of the fourth vacant coordination si

259 s not a good discriminator of the WT; while, Coulombic or reaction field energies perform better depe

260 This non-Coulombic ordering is further enhanced in the presence o

261 We show that Coulombic ordering reduces when the pores can accommodat

262 al neutrality occurs in these liquids due to Coulombic ordering, in which ion shells of alternating c

263 h predicted and observed for highly strained coulombic photonic crystals, suggesting possible applica

264 ed unfavorable total electrostatic energies (Coulombic plus desolvation).

265 r reaction enables electrons to escape their Coulombic potentials on ultrafast time scales.

266 s and monovalent microions that interact via Coulombic potentials to simulations of macroions interac

267 Coulombic recovery decreased as a function of nitrate do

268 ls (MEC and MPPC) achieved approximately 30% Coulombic recovery.

269 first one, dominated by long-range screened Coulombic repulsion (Wigner glass) and a second one, sta

270 d across the octahedral faces, and the Ir-Ir Coulombic repulsion across shared faces that destabilize

271 Higher ion stabilities due to lower Coulombic repulsion and charges being sequestered at hig

272 rmer mutation, designed to remove a possible Coulombic repulsion between E(-3)(NR2B) and Asp-243 (PDZ

273 ced by Glu-161, which introduces a potential coulombic repulsion between enzyme and substrate.

274 r the pairs on the outside--a consequence of Coulombic repulsion between the inner bipyridinium subun

275 Upon oxidation, Coulombic repulsion between the positively charged and m

276 obably a result of the reduced importance of Coulombic repulsion due to the larger size of tin and a

277 tethered duplexes are extended because of a Coulombic repulsion estimated to be 2-5 kT/bp.

278 Coulombic repulsion in the two-dimensional electron syst

279 ns of small molecules and helps overcome the Coulombic repulsion of bringing two cationic species int

280 charge per group becomes less likely due to Coulombic repulsion of like charges.

281 urrounding the helices more than offsets the Coulombic repulsion of parallel arrangements.

282 ar proton redistribution according to simple Coulombic repulsion prior to backbone cleavage into C: a

283 type-II conduction band alignment driven by coulombic repulsion that eliminates non-radiative multi-

284 on several factors that include M-M-C angle, Coulombic repulsion, alkali metal cation size, and the c

285 d dumbbell components gives rise to enhanced Coulombic repulsion, destabilizing the ground-state co-c

286 Despite the unfavorable Coulombic repulsion, the singlet diradical dianion dimer

287 r shape with limited mixing by diffusion and Coulombic repulsion.

288 the spatial evolution of ion packets due to Coulombic repulsion.

289 located near the peptide termini to minimize Coulombic repulsion.

290 -neighbor dipolar coupling interactions, and Coulombic repulsion.

291 ouble reduction is consistent with increased Coulombic repulsion.

292 e distance from one another, thus minimizing Coulombic repulsion.

293 arbon-based analogue, presumably a result of Coulombic repulsions minimizing noncovalent interactions

294 nium radical cation, despite the presence of Coulombic repulsions.

295 A(*-)/D(*+) encounter pair, which outweighs Coulombic stabilization in acetonitrile.

296 to the free A(*-) + D(*+), which opposes the Coulombic stabilization of A(*-)/D(*+).

297 That prediction incorporated only a Coulombic stabilization of the A(*-)/D(*+) encounter pai

298 s strategy of catalysis boosting by means of Coulombic stabilization of the initial Fe(0)-CO2 adduct

299 teractions dominate entropy, and the favored coulombic structure is a charge-ordered state.

300 ic charge analysis provided estimates of the Coulombic work terms associated with ion pairing, DeltaG