ライフサイエンスコーパス: heat transfer

1 ortant for almost all applications involving heat transfer.

2 chnologies that leverage nanoscale radiative heat transfer.

3 d handling, on self-cleaning surfaces and in heat transfer.

4 unding non-polar octane molecules can hinder heat transfer.

5 gap-size-dependent enhancements of radiative heat transfer.

6 s in applications such as fog harvesting and heat transfer.

7 th liquid-infusion for enhanced condensation heat transfer.

8 uding sample preparation, flow reaction, and heat transfer.

9 d methods for controlling small droplets and heat transfer.

10 icant insulating layer that blunts abdominal heat transfer.

11 osity inhibits rapid bubble growth, reducing heat transfer.

12 gered drug release, based on shape-selective heat transfer.

13 ransport that is beneficial for condensation heat transfer.

14 to a reduction of the fuel vapor release and heat transfer.

15 ng fluid to significantly enhance convective heat transfer.

16 ion reactions through a lens of phase change heat transfer.

17 on by coupling crystallization kinetics with heat transfer.

18 ces offer the potential to enhance two-phase heat transfer.

19 ted with heating frequency, thermal mass and heat transfer.

20 unities for quantum materials in controlling heat transfer.

21 y materials, microelectronics, and nanoscale heat transfer.

22 g the contribution from transient conduction heat transfer.

23 hich significantly enhances the condensation heat transfer.

24 gradients, thereby, demonstrating effective heat transfer.

25 ieve a high degree of asymmetry in radiative heat transfer.

26 applications in biotechnology, medicine and heat transfer(1-10).

27 pling across a vacuum and thereby facilitate heat transfer(2-4).

28 ain effective self-cleaning, anti-fouling or heat-transfer abilities in harsh operating environments.

29 A quantum theory of solid-liquid heat transfer accounts for the water-specific cooling en

30 ever, the lack of systematic analysis on the heat transfer across the GaN-BAs interface hampers the p

31 ndings demand modified or even new models of heat transfer across vacuum gaps at nanometre distances.

32 LPT) in quenching are the bottlenecks to the heat transfer advancements.

33 sidence time while preserving the mixing and heat transfer advantages of flow systems.

34 rs increased destruction exergy and enhanced heat transfer, albeit at the cost of efficiency in energ

35 Super-Planckian near-field radiative heat transfer allows effective heat transfer between a h

36 the nozzle-to-laser separation distance, the heat transfer along the printed silver wire is modeled a

37 ns and electrons) in the thermal domain, the heat transfer analogue to the familiar electrical diode.

38 ation involved a systematic investigation of heat transfer, analyte retention, and migration velocity

39 e substantially reduce the thermal radiation heat transfer and achieve one of the lowest high-tempera

40 ere, we develop a biophysical model based on heat transfer and aerodynamic principles to investigate

41 lasma that can ablate tissue with negligible heat transfer and collateral damage to neighboring tissu

42 ning patterns based on numerical modeling of heat transfer and fluid flow in three dimensions.

43 A well-tested numerical heat transfer and fluid flow model is used to compare su

44 ion (VoM-PhyS) framework to simulate coupled heat transfer and fluid flow using a multi-scale voxel m

45 (CO2 photoreduction), anti-fogging surfaces, heat transfer and heat dissipation, anticorrosion, litho

46 the membrane has an insignificant effect on heat transfer and heat recovery, suggesting that membran

47 le surface properties is highly desirable in heat transfer and many other engineering applications.

48 ch catalytic reaction kinetics interact with heat transfer and mechanical buckling to create oscillat

49 ) energy uses convective heating to increase heat transfer and produce deeper, controllable lesions a

50 A polarization-dependent heat transfer and specific power suggests the role of el

51 effect driven by subthermal non-local phonon heat transfer and spectral non-uniform temperature.

52 Using Multiphysics simulation of heat transfer and structural mechanics based on finite e

53 We find a considerable enhancement of the heat transfer and study its dependence on the number of

54 Here, using heat transfer and thermodynamics principles, we show how

55 rophilic or neutral surface for condensation heat transfer and to use the superhydrophobic surface fo

56 tive analyses of the electronics, mechanics, heat-transfer and drug-diffusion characteristics validat

57 ng the generality of symmetry constraints in heat transfer, and clarifying its differences from other

58 odel (Hydrus-1D) for soil water propagation, heat transfer, and diffusive gas transport to explain ob

59 s found that complex coupled fluid dynamics, heat transfer, and electrostatic phenomena within the sa

60 rporating the particle absorption, interface heat transfer, and free carrier absorption was developed

61 elds in optical, microwave, radio, acoustic, heat transfer, and other applications with flexibility a

62 sma protein gradients, temperature and local heat transfer, and washing media were considered in the

63 e, from underwater operation to phase-change heat transfer applications.

64 e range of water-harvesting and phase-change heat-transfer applications.

65 superrepellent surfaces for antifouling and heat-transfer applications.

66 It uses a computerized inverse heat transfer approach based on Pennes's bioheat transfe

67 A data-driven model employing the transient heat transfer approach is developed using a licensed ver

68 The impact of wickability, effective heat transfer area, and liquid pressure on CHF is precis

69 n site density, wettability, wickability and heat transfer area.

70 ncreases linearly with the effective surface heat transfer area.

71 es a general figure of merit for evaporative heat transfer as well as design guidelines for achieving

72 rays of nanofibres, we demonstrate effective heat transfer at critical contacts in electronic devices

73 (MFPAF) rely on optical techniques to probe heat transfer at length scales on the order of the phono

74 l spillover of the liquid cap and asymmetric heat transfer at the freeze front, rotating the freeze f

75 h precise laser engraving supported by rapid heat transfer at the solid-liquid interface.

76 e MHMS has been redesigned to provide better heat transfer away from the sampler and skimmer cones an

77 esigned through the careful consideration of heat transfer, band broadening, and pressure drop.

78 Heat-transfer-based analysis of the data indicates that

79 graphene nanostructures in which noncontact heat transfer becomes a dominant channel.

80 profiling studies revealed starkly different heat transfer behavior from the two shapes of gels.

81 eld radiative heat transfer allows effective heat transfer between a hot and a cold body to increase

82 The ability to enhance or limit heat transfer between a surface and impacting drops is i

83 d-dome digesters buried in the soil to study heat transfer between biogas digester and its surroundin

84 he Boltzmann kinetic equation (BKE) for mass/heat transfer between evaporation and condensation surfa

85 tal studies have demonstrated that radiative heat transfer between macroscopic objects separated by n

86 experiments have demonstrated that radiative heat transfer between objects separated by nanometre-sca

87 Here, we show near-field radiative heat transfer between parallel SiC nanobeams in the deep

88 Polder and Van Hove predicted that radiative heat transfer between planar surfaces separated by a vac

89 presents a computational study of radiative heat transfer between rectangular dielectric membranes t

90 Here, we explore near-field radiative heat transfer between two bodies under time modulation b

91 Here, we show that the radiative heat transfer between two coplanar SiN membranes can be

92 coupled by a trilinear Hamiltonian such that heat transfer between two modes refrigerates the third.

93 thosphere is largely governed by the rate of heat transfer by conduction.

94 terintuitive mechanism of increasing boiling heat transfer by incorporating low-conductivity material

95 A heat transfer calculation showed the crack formation tim

96 At large distances the heat transfer can be described by black body radiation,

97 Here, we show how heat transfer can be utilized to mimic neuron functional

98 ples of thermodynamics, fluid mechanics, and heat transfer can improve future mechanical design itera

99 with dopant, is introduced directly into the heated transfer capillary between the atmosphere and the

100 that gas-phase ion generation occurs in the heated transfer capillary of the instrument in a mechani

101 CPI utilizes a heated transfer capillary with a vacuum ultraviolet tran

102 rease expected by the creation of additional heat transfer channels.

103 Pool boiling Heat Transfer Coefficient (HTC) enhancements on spherica

104 can switch its working states and boost its heat transfer coefficient and critical heat flux in its

105 e that significant changes in the convective heat transfer coefficient are possible, based on wind di

106 rous structure with oil further improves the heat transfer coefficient by an additional 30% to 103 kW

107 demonstrated approximately 100% increase in heat transfer coefficient compared to state-of-the-art d

108 ace structures, our findings revealed varied heat transfer coefficient enhancements, with increases o

109 structures and imparts significantly higher heat transfer coefficient even at high heat flux conditi

110 In our experiments, the cracks improved the heat transfer coefficient from 12 kW/m(2) K for laminar

111 Heat transfer coefficient modeling indicated that convec

112 The convective heat transfer coefficient of the heater is h = 0.014 W.c

113 ions, we obtain permissible range of maximum heat transfer coefficient possible in nucleate boiling a

114 tional device also has a superior convective heat transfer coefficient than do other heaters reported

115 mal conductivity, power density, glass cover heat transfer coefficient, and air inlet temperature.

116 Furthermore, convective heat transfer coefficient, heat exchanger effectiveness,

117 ind into account rely on a forced convection heat transfer coefficient.

118 tion on system-level flow and the convective heat transfer coefficient.

119 by the inlet gas temperature and the overall heat-transfer coefficient in the condensation system.

120 ea is also strongly dependent on the overall heat-transfer coefficient, particularly at higher inlet

121 ergy savings when proper membranes with high heat-transfer coefficients are used.

122 a dramatic increase in near-field radiative heat transfer, comparable to that obtained between bulk

123 ints a way toward solving the volumetric and heat-transfer constraints that limit some other hydrogen

124 Using accurate, empirical heat-transfer correlations, we estimated the length of t

125 tream stability behind ships, aeroplanes and heat-transfer devices.

126 temperature modulation, to measure radiative heat transfer down to gaps as small as two nanometres.

127 It also provides new insights into heat transfer during the industrial freezing and temperi

128 At the same time, heat transfer efficiency is reduced.

129 tic energy results in significantly improved heat transfer efficiency over condensate droplet jumping

130 Heat transfer, electrical potential and light energy are

131 field that are directed to realize efficient heat transfer, eliminating the need for additional trans

132 able nanoparticles to absorb light, generate heat, transfer energy, and re-radiate incident photons.

133 bic surfaces for self-cleaning, condensation heat transfer enhancement and anti-icing applications, m

134 minimization, fluid-structure optimization, heat transfer enhancement and truss optimization.

135 It was found that the LFTFs give substantial heat transfer enhancement compared to nanofluids, where

136 We find that the heat transfer enhancement is dominated by the kinematics

137 We also reveal that the mechanism of heat transfer enhancement is essentially due to the time

138 nt compared to nanofluids, where the maximum heat transfer enhancement of 13% was observed over nanof

139 ature fluctuations, the DRL agent achieves a heat transfer enhancement of up to 38.5%, exceeding the

140 The physics governing heat transfer enhancement on textured surfaces is explai

141 n interesting phenomenon which yields marked heat transfer enhancement over the more explored gravity

142 al fluids (LFTFs) and nanofluids in terms of heat transfer enhancement.

143 d mechanisms including adsorption of DNA and heat-transfer enhancement.

144 These heat transfer enhancements imply that the power density

145 nts from their spatiotemporal evolution with heat transfer estimates and geological observations, we

146 uses a mixture of mined nitrate salts as the heat transfer fluid and storage medium, a two-tank therm

147 ).6H(2)O) is considered as a next-generation heat transfer fluid in solar thermal plants.

148 sing a plain tube with Therminol VP-1 as the heat transfer fluid to validate the CFD results for the

149 essful chemical monitoring of the carnallite heat transfer fluid, an experimental method was develope

150 eceiver tube utilizing Therminol VP-1 as the heat transfer fluid.

151 s, usually by modelling the coupling between heat transfer, fluid dynamics and surface reaction kinet

152 derstanding of its complex physics involving heat transfer, fluid dynamics, and phase changes.

153 Heat transfer fluids such as water, methanol, air and gl

154 perfluorinated alkanes (PFCs) and poly-ether heat transfer fluids, which are persistent greenhouse ga

155 Here we measure radiative heat transfer for large temperature differences ( approx

156 Classical molecular dynamics simulations of heat transfer from a carbon nanotube to a model hydrocar

157 ing is an extremely effective way to promote heat transfer from a hot surface to a liquid due to nume

158 ns (<0.5 mm i.d.), essentially instantaneous heat transfer from the assembly to the mobile phase was

159 power output of the PV cell to the radiative heat transfer from the emitter to the PV cell.

160 e of precession indicates efficient resonant heat transfer from the lattice to coherent magnons.

161 mmunities and is responsible for significant heat transfer from the lithosphere to the ocean.

162 ees C, suggesting the initiation of stronger heat transfer from the North Atlantic to the deep Pacifi

163 s coupling with absorbed water, and that the heat transfer from the water to the mineral phase is ine

164 ks that are key elements in technologies for heat transfer, fuel cells and portable chemical systems.

165 face density produced a strong impediment to heat transfer, giving rise to a thermal conductivity of

166 Flowing two-phase heat transfer has been implemented within microvascular

167 Near-field radiative heat transfer has recently attracted increasing interest

168 expected that this short contact time limits heat transfer; however, the amount of heat exchanged and

169 Moreover, modified combustion (MCE), heat transfer (HTE) and overall thermal efficiencies (OT

170 A one-dimensional model of heat transfer in a single road width wall is created and

171 represents a previously unknown mechanism of heat transfer in addition to the conventional conduction

172 Radiative heat transfer in Angstrom- and nanometre-sized gaps is o

173 ating that conductive models for metamorphic heat transfer in Barrovian terrains are incorrect and mu

174 Here we report studies of radiative heat transfer in few A to 5 nm gap sizes, performed unde

175 enabled elucidation of near-field radiative heat transfer in gaps as small as 20-30 nanometres, quan

176 idity of this theory for modelling radiative heat transfer in gaps as small as a few nanometres.

177 ect has implications for passively enhancing heat transfer in heat exchangers and heat pipes.

178 ions are being developed for ODMPs, mass and heat transfer in osmotic process are becoming better und

179 Heat transfer in solids is typically conducted through e

180 rived from a realistic mathematical model of heat transfer in subduction zones.

181 It also provides platforms to investigate heat transfer in systems with moving components.

182 um are particularly important for radiative heat transfer in the ambient environment, because of the

183 eoretical thermodynamic analysis of mass and heat transfer in the membrane condensation system shows

184 scovers optimal control policies to maximize heat transfer in turbulent Rayleigh-Benard convection.

185 We study the heat transfer in two countermoving media and show that t

186 y associated with increased conductive inner heat transfer, indicated by an increased CBT- proximal b

187 Here we experimentally demonstrate heat transfer induced by quantum fluctuations between tw

188 d thus greatly deepen the extent of downward heat transfer induced by TCs.

189 Its heat transfer into both the midlatitude South Indian Oce

190 , we demonstrate that Er(3+) acts to enhance heat transfer into the Er-PVDF film due to its excellent

191 Measuring and characterizing radiant heat transfer is a critical component of both building e

192 onon-mediated both in-plane and out-of-plane heat transfer is clarified for this prospective heterobi

193 Accurate monitoring of boiling heat transfer is critical for the safety and efficiency

194 Enhancing condensation heat transfer is important for broad applications from p

195 in electrical conduction, active control of heat transfer is much more challenging.

196 The rate of heat transfer is reduced significantly with increasing t

197 approach the physical limit of flow boiling heat transfer is reported.

198 Our observations show that lava-snow heat transfer is slow, and that styles of lava propagati

199 Heat transfer is used in chemical processing, power gene

200 high heat flux conditions, in which boiling heat transfer is usually deteriorated due to the develop

201 Effective control of heat transfer is vital for energy saving and carbon emis

202 iven spreading factor, the small fraction of heat transferred is controlled by two dimensionless grou

203 When mass and heat transfer kinetics are limited, conditions that more

204 ated for both limited and unlimited mass and heat transfer kinetics in the thermal separation stage.

205 In the case of unlimited mass and heat transfer kinetics, the energy efficiency of the sys

206 nce to unraveling the breakdown of classical heat transfer laws, far-field optical temperature mappin

207 The Scholander-Irving (S-I) model of heat transfer lays the foundation for explaining how end

208 The column is connected through a heated transfer line to a microfabricated differential m

209 A novel Nichrome wire-heated transfer line was developed to ensure that the ca

210 e generator to an exposure chamber through a heated transfer line.

211 able memory effects were associated with the heated transfer line.

212 tem behavior, particularly the timescales of heat transfer linked to the ocean.

213 s and could supplement conventional metallic heat-transfer materials, which are used in applications

214 We study this heat transfer mechanism using distinct control knobs to

215 study to directly model a metropolitan scale heat transfer mechanism, we find both enhanced tree cano

216 nflated uncertainties when investigating bio-heat transfer mechanisms and/or performing sophisticated

217 lts highlight the relevant role of different heat transfer mechanisms between MI and IM interfaces: a

218 anced electronic systems depend on efficient heat transfer mechanisms for achieving high power densit

219 nometre-scale distances while avoiding other heat transfer mechanisms, namely conduction.

220 also discuss the advantages of using liquid heat-transfer media as compared to air as the heat-trans

221 eat-transfer media as compared to air as the heat-transfer media.

222 lumn linear velocity for both air and liquid heat-transfer media.

223 um chip to measure thermal changes using the heat-transfer method (HTM).

224 ether roasting techniques based on different heat transfer methods (hot air and infrared), differentl

225 ablishment of tunable, ultra-high efficiency heat transfer/mixing systems.

226 ter-energy industries owing to its efficient heat transfer mode.

227 tigated the gauge potential formulation of a heat transfer model in a non equilibrium system within c

228 In this work, a heat transfer model is developed for thermally-driven ma

229 ge thresholds were compared to a theoretical heat transfer model of pulsed laser-irradiated nanoparti

230 oiting the time lags and the one-dimensional heat transfer model of soils, we estimate the ALTs.

231 ynthetic Aperture Radar) observation and the heat transfer model of soils.

232 lag was corroborated using a one-dimensional heat-transfer model, which provided insight into the cha

233 d with salt penetration, water migration and heat transfer models, can be used to dynamically simulat

234 ynamics to describe the convergence of these heat transfer modes and the transition from one to the o

235 he boundary between the two most fundamental heat transfer modes, heat conduction by phonons and radi

236 ns the current finding by revealing that the heat transfer modification and enhancement are mainly at

237 ics simulations coupling electromagnetic and heat transfer modules demonstrate that during pulsed las

238 s well established that near-field radiative heat transfer (NFRHT) can exceed Planck's blackbody limi

239 ve experimentally shown near-field radiative heat transfer (NFRHT) exceeding the far-field blackbody

240 presents negligible resistance to conduction heat transfer normal to it and very large resistance alo

241 y diagnostic is the efficiency of convective heat transfer (Nu).

242 We achieve an enhancement of heat transfer of almost two orders of magnitude with res

243 e for understanding shear-flow and anomalous heat transfer of NS associated non-equilibrium aggregati

244 ated using screen printing of electrodes and heat transfer of patterned wax paper onto filter paper.

245 also show a 30-40% increase in condensation heat transfer on copper, as a result of the ability of t

246 as a wave-like (in contrast with diffusion) heat transfer, or energy propagation, in a gas of quasi-

247 ngles and high nucleation densities for high heat transfer performance have been typically neglected.

248 result, we can rapidly and reversibly alter heat transfer performance up to an order of magnitude.

249 ing phenomena and enhancing nucleate boiling heat transfer performance.

250 r state-of-the-art calculations of radiative heat transfer, performed within the theoretical framewor

251 A description of mass and heat transfer phenomena is provided and fundamental prin

252 From a heat transfer point of view, it was observed that the th

253 urier theory for analysing three-dimensional heat transfer problems in systems with an interface.

254 The applicability of Fourier's law to heat transfer problems relies on the assumption that hea

255 ce enhancement of the two-phase flow boiling heat transfer process in microchannels through implement

256 of experiments and theory, we show that the heat transfer process on superhydrophobic surfaces is in

257 sorption, LiCl@HGAFs experience an efficient heat transfer process, with a heat storage capacity of 6

258 cement in boiling and quenching phase-change heat transfer processes by nanoscale surface texturing c

259 dielectric materials typically exhibit poor heat transfer properties due to the dynamics of phonon t

260 ives could provide by enhancing the mass and heat transfer properties, acting as co-catalysts, or imp

261 and optimize fundamental fluid mechanics and heat transfer properties.

262 initial moisture contents increase, the soil heat transfer rate and bearing capacity decreases after

263 oxy results in a greater than 5x increase in heat transfer rate at a given superheat temperature.

264 Order of magnitude variation in heat transfer rates and cellulose particle lifetimes was

265 s the nucleation potential of the surface to heat transfer rates has been developed and it successful

266 tunable design parameter to control particle heat transfer rates in industrial biomass reactors.

267 rse opal coated copper tubes maintained high heat transfer rates when the experiments were repeated >

268 ls for potential applications in sensing and heat transfer, respectively.

269 Flow reactors enhance the mass and heat transfer, resulting in rapid reaction mixing, and e

270 A micro-heat transfer sensor was deployed to acquire the ISS pro

271 of the conductive filament and the amount of heat transferred several resistance-changing effects are

272 ate model of Laser Powder Bed Fusion (L-PBF) heat transfer simulation.

273 ious bulk optical spectroscopy and nanoscale heat transfer studies, revealing the different mechanism

274 Phase-change heat transfer such as boiling and evaporation has been w

275 mal energy conversion calculations including heat transfer suggest that amorphization is a solid-stat

276 t the vapor phase lateral expansion over the heat transfer surface and actively control the surface w

277 g, solar thermo-photovoltaics and nano-scale heat transfer systems.

278 ons such as atmospheric water harvesting and heat transfer that uses water as a refrigerant, replacin

279 currents predicted from near-field radiative heat transfer theory.

280 n panels, nanotextured surfaces for enhanced heat transfer, thermal and electrical insulation films,

281 asitic power consumption and allow efficient heat transfer through good thermal contacts with the hea

282 Convective heat transfer through jugular venous return and the circ

283 : within three days, a high fat diet reduces heat transfer through skin.

284 mammals, generally by estimating conductive heat transfer through their blubber layer.

285 M minimizes thermal resistance by convective heat transfer to a constantly moving droplet in direct c

286 There was no increase in heat transfer to a tooth analogue when the high volume e

287 a Leidenfrost phenomenon, which impedes the heat transfer to cool the liquid, when the liquid drople

288 The condition of heat transfer to lignocellulosic biomass particles durin

289 ed within the individual nanostructures when heat transfer to neighbouring nanostructures and the env

290 bstitution by CF, GF and RF in bread reduces heat transfer to the dough center by about 21%, 35% and

291 igh optical absorption of the CNTs and rapid heat transfer to the polymer upon excitation by pulsed l

292 ced within the test system without increased heat transfer to the tooth.

293 rared emission to accomplish large and rapid heat transfer tuning in response to human perspiration v

294 Our set-up enables effective heat transfer using a liquid at previously unattainable

295 efficient modeling indicated that convective heat transfer was suspended, probably by suppressing gil

296 important in industrial applications such as heat transfer, water collection, and particle separation

297 ve pressures (-1.0 MPa or lower), continuous heat transfer with the evaporation of liquid water at ne

298 w-type conical turbulence promoters enhanced heat transfer, with the best performance achieved at Per

299 ance detector, multiphysical modeling of the heat transfer within the conductivity cell was performed

300 ance due to insufficient control of mass and heat transfer within the interfacial reaction zone.