ライフサイエンスコーパス: Nernst

1 Nernst analyses suggest that the reduction of CODH from

2 membrane potential from becoming the Ca(2+) Nernst potential in <1 ms.

3 The titrations fit a Nernst equation for a one-electron reaction and were nea

4 formed at maximum current density revealed a Nernst-Monod response with a half saturation potential (

5 nts and electrophoretic mobilities satisfy a Nernst-Einstein relation in which the effective charge o

6 representative two-electron redox system; a Nernst slope of -30.8 mV was obtained.

7 antum) model, mathematically equivalent to a Nernst distribution for one redox energy level, redox si

8 on and withdrawal of NH(4)(+) conformed to a Nernst equation modified to include realistic NH(4)(+) p

9 m) with multiple layers of active cells, and Nernst-Monod behavior support extracellular electron tra

10 hase electric potentials known as Donnan and Nernst potentials.

11 hmark problems (involving, e.g., Fickian and Nernst-Planck diffusion, isotope fractionation, advectio

12 ries of strikingly large zero-field Hall and Nernst effects in antiferromagnets Mn(3)X (X = Sn, Ge) h

13 es in simulation via solving the Poisson and Nernst-Planck equations, the SCD and therefore the surfa

14 x) by measuring both magneto-resistivity and Nernst effect on ultrathin flakes (<=2 unit-cell).

15 and quantum oscillations in the Seebeck and Nernst effect.

16 Temperature-dependent Hall, Seebeck, and Nernst measurements consistently indicate the existence

17 ic coefficients, such as the thermopower and Nernst coefficient, are greatly enhanced over their zero

18 Anomalous Nernst effect (ANE), converting a heat flow to transvers

19 In magnetic materials, an anomalous Nernst effect (ANE) is possible in a zero magnetic field

20 thin films grown on Si manifest an anomalous Nernst effect with a finite spontaneous signal at zero m

21 ions and a new pathway to enhanced anomalous Nernst effect for transverse thermoelectrics.

22 ion contains the contribution from anomalous Nernst effect (ANE).

23 her exhibits large anomalous Hall, anomalous Nernst, and anomalous thermal Hall effects, all of which

24 we report the observation of large anomalous Nernst effect and anomalous thermal Hall effect in this

25 Here we report a large anomalous Nernst effect in antiferromagnetic SrIr(0.8)Sn(0.2)O(3)

26 A large anomalous Nernst effect is essential for thermoelectric energy-har

27 hermoelectric performance based on anomalous Nernst effect.

28 culations of the momentum-resolved anomalous Nernst conductivity, highlighting the contributions of a

29 microscopy using the time-resolved anomalous Nernst effect (TRANE).

30 The observed spontaneous anomalous Nernst coefficient reaches the value of 0.26 muV/K with

31 Recently, an HFS utilizing the Anomalous Nernst Effect (ANE) has been proposed garnering signific

32 hermoelectric generation using the anomalous Nernst effect (ANE) has great potential for application

33 s of the electronic structure, the anomalous Nernst effect (ANE) originates from the Berry curvature

34 The anomalous Nernst effect generates a voltage transverse to an appli

35 ymmetry-class of altermagnets, the anomalous Nernst effect is possible despite the compensated collin

36 a large anomalous Hall effect, the anomalous Nernst effect, and the topological Hall effect (THE).

37 gnetism in WTe(2) manifests in the anomalous Nernst effect, anomalous Hall effect as well as anisotro

38 ent combined with detection of the anomalous Nernst effect.

39 age responses closely resemble the anomalous Nernst responses to AC temperature gradient generated by

40 nst and GHK equations, (b) reporting of both Nernst-selectivity and GHK-selectivity along with soluti

41 try priors including the Butler-Volmer (BV), Nernst and diffusion equations on the backbone of neural

42 ry generated magnetic fields are advected by Nernst flows and anisotropic pressure effects dominate t

43 The theory of this method is described by Nernst-Planck-Poisson finite element simulations, and bo

44 For ideal gas mixtures we derive the classic Nernst-Planck equation.

45 Here, we report the discovery of colossal Nernst power factor of 3800 x 10(-4 )W m(-1) K(-2) under

46 Combining Nernst and spin Seebeck effect in bulk materials would e

47 rcuit potential (OCP) were used to construct Nernst plots to evaluate the applicability of the drople

48 The coupled Nernst-Planck equations (multi-ion model, MIM) for the c

49 cribed quantitatively by the one-dimensional Nernst-Planck equation for mass transport over the full

50 d by resolving the coupled three-dimensional Nernst-Planck, Poisson, and Navier-Stokes equations.

51 lectrostriction and analyzed using the Drude-Nernst equation.

52 so develop equations for an electrochemical (Nernst) transport mechanism for the promoter, and descri

53 Thus, the one-electron Nernst behavior can be interpreted as the sum of two sep

54 acetyl-CoA synthesis exhibited one-electron Nernst behavior, and the effects of pH on the observed m

55 to the magnetic field induced Ettingshausen-Nernst effect.

56 gh the membrane is described by the extended Nernst-Planck equation, with the consideration of fricti

57 A variable-electric-field Nernst-Planck electrodiffusion model was used, with two

58 Reported is a zero-field Nernst effect in a newly discovered hard-ferromagnetic k

59 ransport in battery cathode materials, e.g., Nernst-Einstein conduction, cannot explain the measured

60 ellular GSH, preserved the intracellular GSH Nernst potential, and reduced apoptosis caused by oscill

61 Recently found anomalous Hall, Nernst, magnetooptical Kerr, and spin Hall effects in th

62 oating, the Li(+) ISE sensors possess a high Nernst slope (59.14 mV/dec), rapid response (<10 s), and

63 -4 )W m(-1) K(-2) under 5 T at 25 K and high Nernst figure-of-merit of 71 x 10(-4 )K(-1) under 5 T at

64 entration changes according to the Kirchhoff-Nernst-Planck formalism.

65 otentiometry is determined by the well-known Nernst equation.

66 his notion by observing an anomalously large Nernst effect in a range of conducting polymers.

67 omagnetic performance is attributed to large Nernst thermopower and longitudinal electrical conductiv

68 By leveraging Nernst measurements, we provide direct evidence of ferro

69 stry on the rhenium compound yields a linear Nernst plot with an n value of 0.99 and E degree' of 0.0

70 A maximum Nernst thermopower of ~3 uV K(-1) at 80 K in zero field

71 A modified Nernst-Planck model incorporating ion hydration and elec

72 p is <6.0 and p is >8.5 in a proton-modified Nernst equation.

73 tion of electro-diffusion processes, namely, Nernst-Planck-Poisson (NPP) model to allow the descripti

74 n protein diffusion and kD in the context of Nernst-Planck theory.

75 ions through the gap junction pore based on Nernst-Planck equations for ion concentrations and the P

76 and hexagonal boron nitride exhibit perfect Nernst selectivity such that only protons can permeate t

77 al photocurrent is generated through a photo-Nernst type effect with its direction controlled by the

78 A Poisson-Nernst-Planck (PNP)-steric model of arginines and a mech

79 A Poisson-Nernst-Planck/density functional theory model of RyR is

80 nted as featureless dielectrics, and Poisson-Nernst-Planck (PNP) electrodiffusion theory in which bot

81 have performed Langevin dynamics and Poisson-Nernst-Planck calculations to simulate detection of prot

82 um approaches (Poisson-Boltzmann and Poisson-Nernst-Planck theory) have been also employed.

83 This claim is buttressed by Poisson-Nernst-Planck calculations that predict a high single-ch

84 simulation of unsteady fully coupled Poisson-Nernst-Planck (PNP) equations.

85 element method to solve the coupled Poisson-Nernst-Planck and Navier-Stokes equations under unsteady

86 the pore is described by the coupled Poisson-Nernst-Planck and the Stokes equations that are solved s

87 inuum model, composed of the coupled Poisson-Nernst-Planck equations for the ionic mass transport and

88 gy for solving the three-dimensional Poisson-Nernst-Planck equations is used to compute current-volta

89 model for RNA with the 3-dimensional Poisson-Nernst-Planck formalism for electric fields within prote

90 mics (GCMC/BD) and three-dimensional Poisson-Nernst-Plank (3d-PNP) electrodiffusion algorithms offer

91 ion by utilizing the one-dimensional Poisson-Nernst-Plank model to determine the voltage profile of s

92 We use an extended Poisson-Nernst-Planck (PNP2) theory to compute (mean) Coulombic

93 We show that the fluctuating Poisson-Nernst-Planck (PNP) equations for charged multispecies d

94 eory, termed Potential-of-Mean-Force-Poisson-Nernst-Planck theory (PMFPNP), to compute ion currents.

95 The continuum model is a generalized Poisson-Nernst-Planck (GPNP) system where an activity coefficien

96 olyte-filled pore using the modified Poisson-Nernst-Planck and Navier-Stokes equations.

97 al simulations based on the modified Poisson-Nernst-Planck model and showed that the results agree wi

98 ty assumptions are applied to obtain Poisson-Nernst-Planck-type equations or a generalized Ohmic law.

99 roach utilizes a modified version of Poisson-Nernst-Planck (PNP) theory, termed Potential-of-Mean-For

100 a continuum model based on a set of Poisson-Nernst-Planck and Stokes-Brinkman equations was adopted.

101 ained from the numerical solution of Poisson-Nernst-Planck equations in axisymmetric domain.

102 Then, by solving Poisson-Nernst-Planck and Navier-Stokes equations, we determined

103 algorithm is developed to solve the Poisson-Nernst-Planck (PNP) equations for ion transport through

104 were analyzed by an extension of the Poisson-Nernst-Planck (PNP) formulation of electrodiffusion, whi

105 me techniques were used to solve the Poisson-Nernst-Planck equation, and a dual Delaunay-Voronoi mesh

106 in extracellular fluid based on the Poisson-Nernst-Planck equations of electrodiffusion.

107 e-grained models of polymers and the Poisson-Nernst-Planck formalism for ionic current.

108 nd numerous simulations based on the Poisson-Nernst-Planck formalism provide details of the observati

109 VB simulation data combined with the Poisson-Nernst-Planck theory indicates that the triply protonate

110 a channel is described by a theory (Poisson-Nernst-Planck, PNP) that computes the average electric f

111 rin channels is also estimated using Poisson-Nernst-Planck theory for both the Grotthuss shuttling ex

112 he inward current was close to the predicted Nernst equilibrium potential for Na+.

113 re linar and reversed close to the predicted Nernst potential for K+.

114 ence rises proportionally but not so for RED Nernst potential, which has logarithmic dependence on th

115 -) concentrations together with the relevant Nernst equation resolved the tetrathionate/thiosulfate r

116 Here, we present a study of angle-resolved Nernst effect in bismuth, which maps the angle-resolved

117 pin caloritronics phenomena such as the spin Nernst effect and serves as a reference for theoretical

118 chirality of the condensate induces the spin Nernst effect, where a spin current is generated perpend

119 We accomplish this by comparing the spin Nernst magneto-thermopower to the spin Hall magnetoresis

120 The spin Nernst ratio for Bi(2)Se(3) is the largest among all mat

121 a lower bound for the magnitude of the spin Nernst ratio is -0.61 +/- 0.11.

122 .26 muV/K with the corresponding spontaneous Nernst conductivity of 0.22 A/(K . m).

123 The observed spontaneous Nernst thermopower quickly reaches the sub-muV/K level b

124 magnetic actinide materials can host strong Nernst and Hall responses due to their combined correlat

125 The Nernst-Planck equations are simplified to the Debye-Falk

126 ng currents at membrane potentials above the Nernst equilibrium potential for Cl(-) and thus can be u

127 In addition, the Nernst signal displays a sign anomaly in the gap-inverte

128 it could react with the metal and affect the Nernst potential at the metal-solution interface.

129 We further analyze the Nernst signal above T(c) in the framework of Gaussian su

130 sing information from the literature and the Nernst-Einstein conductivity equation, it was shown that

131 for these responses closely approximated the Nernst equilibrium potential for K(+).

132 Zero-current potentials approximated the Nernst for Cl-, and rectification usually followed that

133 hibit sensitivities to pH changes beyond the Nernst limit.

134 Classically, this process is driven by the Nernst effect in bulk solids, wherein a magnetic field g

135 with the theoretical value predicted by the Nernst Equation (-59.2 mV pH(-1)).

136 ty with the voltage output determined by the Nernst equation and proportional to the logarithm of the

137 e Ca2+-dependent current as predicted by the Nernst equation for a K+-selective current.

138 in agreement with the value predicted by the Nernst equation for a potassium conductance; serotonin o

139 ternal Cl- concentration as predicted by the Nernst equation for chloride ions.

140 with changes in [Cl-]i, as predicted by the Nernst equation.

141 in a greater quantity than predicted by the Nernst equation.

142 ding membrane potentials as predicted by the Nernst equation.

143 vity of ion-selective sensors limited by the Nernst equation.

144 transfer (CT)-IT system have considered the Nernst equation for the CT, while there is no empirical

145 rought membrane potentials closer to EK (the Nernst potential for K+ ions), suggesting activation of

146 ansport rates were analyzed by employing the Nernst-Planck equation, modified to account for electric

147 selectivities in nanopores often employs the Nernst or Goldman-Hodgkin-Katz (GHK) equation to interpr

148 ntly higher sensitivity which can exceed the Nernst limit.

149 implicitly assumes the same symmetry for the Nernst and Hall coefficients, which is however not neces

150 ion, one obtains boundary conditions for the Nernst-Planck equation that guarantee that the pore is o

151 ing alkaline electrolyte originates from the Nernst potential of the pH gradient layer at the cathode

152 flow in a driving temperature gradient (the Nernst effect), in magnetic fields up to 45 tesla.

153 duced as they diffuse down the gradient (the Nernst effect).

154 ppa-(BEDT-TTF)(2)X family, we reveal how the Nernst effect, a sensitive probe of superconducting phas

155 porating enzymatic rate expressions into the Nernst equation was derived to explain the observed pote

156 henomenon in many solid-state materials, the Nernst effect has yet to be observed in conducting polym

157 me batch of ultrathin flakes, we measure the Nernst effect via on-chip thermometry.

158 ic transport in this endeavor, we modify the Nernst-Planck equation by incorporating an additional el

159 individual ion-water clusters still obey the Nernst-Einstein relation, the overall relation breaks do

160 -induced formation and transformation of the Nernst diffusion layer, demonstrating that pulsed voltag

161 ology because the transverse geometry of the Nernst effect should enable efficient, large-area and fl

162 Formal analysis of the Nernst equation reveals that reduction potential contain

163 Fits of the Nernst equation to the corresponding lag-vs-potential pl

164 ectrodes ideally operate on the basis of the Nernst equation, which predicts less than 60- and 30-mV

165 Application of the Nernst-Einstein equation to these data gives the followi

166 variation of the convective component of the Nernst-Plank equation for flux and, to lesser extent, di

167 ow-power thermoelectric devices based on the Nernst effect and are thus valuable for the comprehensiv

168 rom the first-order predictions based on the Nernst equation to the implicit inclusion of second-orde

169 In a thermoelectric device based on the Nernst geometry, an external magnet is required as an in

170 Such electroanalysis, based on the Nernst-Donnan equation, has been predominantly performed

171 ), Ca(2+), Mg(2+), and SO4(2-)) based on the Nernst-Planck equation, and uses it for permeate and ret

172 We adopt a model based on the Nernst-Planck theory, that requires only three input par

173 In this paper, the Nernst equation is used to simultaneously calculate the

174 ithin the Landau's Fermi-liquid picture, the Nernst coefficient has demonstrated to be proportional t

175 e predicted for a fixed probe by solving the Nernst-Planck equation and that the ac response can also

176 ns that cross the channel and by solving the Nernst-Planck equation yield consistent results, indicat

177 Specially, the Nernst coefficients in these doped polymers exceed the F

178 dicularly applied magnetic field, termed the Nernst effect, has promise for thermoelectric applicatio

179 We find that the Nernst signal is anomalously enhanced at temperatures as

180 tube porins (CNTPs) and demonstrate that the Nernst-Einstein relation in these channels breaks down b

181 ited by the value predicted according to the Nernst equation and inversely proportional to the charge

182 which equilibrates in cells according to the Nernst equation and provides a numerical, replicable est

183 -500 mV) fit a function corresponding to the Nernst equation with a midpoint potential of -316 mV.

184 nd the potential changes with respect to the Nernst equation.

185 e potential in the solution according to the Nernst equation.

186 tential that varies with pH according to the Nernst equation.

187 (GSSG) and calculated E(h) according to the Nernst equation.

188 potentials has been shown to be equal to the Nernst equilibrium potential of the most permeant inorga

189 channels in activating well negative to the Nernst potential for protons, E(H).

190 us proton channels open only positive to the Nernst potential for protons, E(H).

191 orates these interactions and reduces to the Nernst-Einstein conduction under dilute conditions.

192 e Goldman-Hodgkin-Katz (GHK) solution to the Nernst-Planck equation for transport across the membrane

193 rchers arbitrarily choose whether to use the Nernst or GHK equation and overlook the significant diff

194 We used the Nernst-Planck equation as the mass balance equation to d

195 olutions in which they reside when using the Nernst and GHK equations, (b) reporting of both Nernst-s

196 culated to be -275.4 +/- 0.3 mV by using the Nernst equation and the Keq for the equilibrium of the r

197 nd GSSG, and the calculation of Eh using the Nernst equation.

198 nalyzed as a function of potential using the Nernst equation.

199 um CRP speciation and calculations using the Nernst equation.

200 t is converted to a resistivity by using the Nernst-Einstein relation.

201 fusion we encounter a situation in which the Nernst-Planck contribution to diffusion differs by sever

202 ion approach is first developed in which the Nernst-Planck equation is used to characterize axial ion

203 Cys, CySS, GSH, and GSSG were used with the Nernst equation to calculate the redox states.

204 allows DeltaPsi(m) to be calculated with the Nernst equation, but this has proven difficult in practi

205 activity in the sample in agreement with the Nernst equation.

206 in whole vacuole recordings shifted with the Nernst potential for Cl-and vanished in glutamate.

207 Combined with the Nernst-Einstein relation, these diffusion results constr

208 For over 100 years, the Nernst-Einstein relation has linked a charged particle's

209 solution potential and that it's theoretical Nernst equation of E(H)[mV] = 855 - 177 pH - 59 log [Fe(

210 The transverse thermoelectric (Nernst) effect is a powerful probe for studying the elec

211 The large and unsaturated Nernst thermopower is the result of the combination of h

212 In this study, we utilize Nernst-Planck based models for continuous flow ED and co

213 alized model that couples the Butler-Volmer, Nernst-Planck, and Poisson equations.

214 of superconducting fluctuations, the vortex-Nernst effect, we find that a fluctuating regime develop

215 We fabricate a FM alloy with zero Nernst coefficient to mitigate the ANE contamination of