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1 annel, mitigating the deleterious effects of Joule heating.
2 cesses to the synthesis of graphene by flash Joule heating.
3 catalyst deactivation compared to Continuous Joule Heating.
4 FAs by simultaneously combining pH swing and joule heating.
5 round the conductor, primarily influenced by joule heating.
6 cooling mechanism to mitigate the impacts of Joule heating.
7 temperature of the hot electrons through the Joule heating.
8 ing-to-conducting phase transition driven by Joule heating.
9  at strains as high as 140%, and can support Joule heating.
10  the sensor recovery time, probably by local Joule heating.
11 e atomic scale, for graphitic nanoribbons by Joule heating.
12 ot cause significant intra- or extracellular Joule heating.
13 p velocity while minimizing dissipation from Joule heating.
14 rmometer, we mapped the thermal expansion of Joule-heated, 80-nanometer-thick aluminum wires by preci
15 rectly drive nanocrystal nucleation in flash Joule heating, an insight that may inform future Joule h
16 rbed RF energy in brain tissue converts into Joule heat and affects the nuclear magnetic shielding an
17 me was 20 min for careful operation to limit Joule heating and electroendosmosis.
18                                       During Joule heating and electron beam irradiation, carbon atom
19             Paper based ITP is challenged by Joule heating and evaporation because it is open to the
20  helps suppress the negative impacts such as Joule heating and gas bubble evolution from common nanos
21                                        Here, Joule heating and inefficient thermal dissipation are sh
22  is typically considered to be the result of Joule heating and is overlooked without an appropriate a
23 t of electroporation protocols that minimize Joule heating and maximize cell viability.
24               In this study, we investigated Joule heating and pH as parameters controlling the dewat
25 ven control of magnetization, which involves Joule heating and power dissipation.
26 constructive interference effect between the Joule heating and temperature-dependent resistance effec
27                 Electromagnetic mechanism of Joule heating and thermal conduction on conductive mater
28 at the pulse-induced transition is driven by Joule heating, and that the pulse-induced state correspo
29  surface electrodes for actuation, localized Joule heating, and thermistic temperature sensing.
30  0.1 MV.cm(-1), indicating that effects from Joule heating are minor.
31 temperature gradients resulting from intense Joule heating at constrictions between grains.
32 the unwanted side effects of electrolysis or joule heating at electrodes compared to DC electroporati
33                         Here, we introduce a joule heating-based platform technology, whereby biosyst
34 llent phase engineering ability of the flash Joule heating by broadly tunable energy input that can e
35                                Additionally, Joule heating can potentially induce thermal flow and mo
36 lable exothermic reactions in electrodes and Joule heating can result in the catastrophic failures su
37 oic heterostructures(9-12), which suppresses Joule heating caused by switching currents and may enabl
38 flux and the responding electric energy, the Joule heating, consumed in the cell membrane, as well as
39 periment are a critical aspect in iDEP since Joule heating could lead to various detrimental effects
40        The experimental findings reveal that Joule heating could result in an excessive temperature r
41                                   We use the Joule heating created by current spikes to trigger the i
42  nm, allowing us to identify the presence of Joule heating, current crowding and thermoelectric heati
43 paration fields can be applied before excess Joule heating degrades the separation.
44                  Both electrical current and Joule heating diminish with increasing pressure, and the
45 vity of the copolymer film permits efficient Joule heat dissipation and, accordingly, excellent cycli
46              The temperature rise due to the Joule heating effect was measured using a thermoreflecta
47 he conductive carbon substrate, known as the Joule-heating effect.
48            The ultrafast sintering method by Joule heating effectively shorten the sintering time fro
49                                              Joule heating effects are expected to be acute in open m
50                      In addition, a model of Joule heating effects in the microdevice during operatio
51 By a comparison with the shock field-induced Joule heating effects on cell membranes, the field-induc
52 elongating surface considering radiation and Joule heating effects significant.
53 yer to produce chiroptical responses and the Joule heating electrode to electrically program phase ch
54 film carbon nanotube (CNT)/polymer composite Joule heating element can prevent CNT degradation in ion
55          We develop numerical simulations of Joule heating-enhanced diffusion during electrophoresis
56 perature-controlled electrodes revealed that Joule heating enhances water removal by increasing evapo
57  intrinsically affected by the generation of Joule heating, entailing a drop in viscosity and possibl
58 f attolitres (10(2)-10(5) nm3) of polymer by Joule heating, extremely non-uniform electric field grad
59                     Here, we introduce flash Joule heating (FJH) combined with chlorination (FJH-Cl(2
60 ocess (~3000 degrees C, ~1 s) based on flash Joule heating (FJH) for activating wastes to improve REE
61 e, we report a solvent- and water-free flash Joule heating (FJH) method combined with magnetic separa
62 -derived flash graphene (AFG), via the flash joule heating (FJH) process.
63                We use here a pulsed dc flash Joule heating (FJH) strategy that heats the black mass,
64 umn zone that can be heated up to 3000 K via Joule heating, followed by melting on the order of milli
65 ted effects such as transverse diffusion and Joule heating for a given faceted prism.
66 e insensitivity allow for compression-stable Joule heating for wearable thermal management.
67                 The attractive advantages of Joule-heat-free transmission of information, utilization
68        Here we describe a flash-within-flash Joule heating (FWF) technique-a non-equilibrium, ultrafa
69                    In the former, controlled Joule heating generated by a voltage-biased quantum poin
70                                        Flash Joule heating has emerged as an ultrafast, scalable, and
71 mechanical coupling (>600% strain); ii) with Joule-heated healing and reprocessability; iii) with ele
72                             Instead of local Joule heating, however, the dissipation mechanism compri
73  viscous dissipation, thermal radiation, and Joule heating impacts are also considered.
74 rated a phase change memory effect in KBS by Joule heating in a technologically relevant vertical mem
75 ing temperature distributions resulting from Joule heating in a variety of microfluidic circuits that
76 trogen species through high-power electrical joule heating in ammonia gas, leading to n-type electron
77 erromagnetic-to-ferromagnetic transition via Joule heating in FeRh wires.
78     It generates sound thermoacoustically by Joule heating in graphene.
79 locally up to 1000 K, validating the role of Joule heating in resistive switching.
80 ts were attributed to less gas formation and Joule heating in SFE.
81 usly away from the cooling junction, so that Joule heating in the bulk element does not diminish the
82 espite this, the roles of electric field and Joule heating in the switching process remain controvers
83 tallisation energy, which is comparable with Joule heating induced by a controlled current introducti
84 e attribute the oriented growth to the local Joule-heating induced by electrical bias near the interf
85                                              Joule-heating induced conductance-switching is studied i
86  of graphene in the air first shows signs of joule heating-induced cleaning followed by rupturing of
87 n of suspended few-layer graphene by in situ Joule-heating inside a transmission electron microscope.
88 alyte diffusivity due to autothermal runaway Joule heating is a dominant mechanism that reduces separ
89 olvent-free and sustainable process by flash Joule heating is disclosed to recover precious metals an
90                              In this method, Joule heating is generated by applying high electric pow
91 rmore, elevated device temperature caused by Joule heating is shown as an important factor contributi
92 urrent electrothermal flow (ACET) induced by Joule heating is utilized to transport biologically rele
93 gh as 600 V/cm could be applied with minimal Joule heating (<2 degrees C).
94                                     However, Joule heating may cause significant temperature rises, w
95             This heat can be generated via a Joule heating mechanism or high power laser pulses.
96 les, which are synthesized via a novel rapid Joule heating method, can serve as nanoseeds to direct t
97                            By optimizing the Joule heating method, ultrafine Ag nanoparticles ( appro
98 ilization on carbon supports through in situ Joule heating method.
99 etry reveals a temperature gradient across a joule-heated microstructure that is undetectable with di
100                 We validate the mechanism of Joule heating modulated competition between the Ruderman
101 insights into heat dissipation mechanisms of Joule heated nanotube devices that are more complex than
102 y in the crossover channel indicates that no Joule heating occurs at voltages of at least 2.0 kV.
103 bot with multiple crawling modes, enabled by joule heating of a patterned soft heater consisting of s
104 tron thermal microscopy to detect the remote Joule heating of a silicon nitride substrate by a single
105 a ~65 m(2) g(-1)) by a pulsed direct current Joule heating of gamma-Al(2)O(3).
106                      Here we show that flash Joule heating of inexpensive carbon sources-such as coal
107 plications in nanoscale electronics, because Joule heating of interconnecting wires is a major proble
108 ectrically induced actuation associated with Joule heating of the matrix when a current is passed thr
109 uced by a conventional REIMS mechanism using Joule heating of the tissues, which was consolidated by
110 e impact of MHD and viscous dissipation with joule heating on convective stretching flow of dusty tan
111 e heating, an insight that may inform future Joule heating or other electrical synthesis strategies.
112 le-step electrified approach utilizing Rapid Joule Heating over an H-ZSM-5 catalyst to efficiently de
113                 Negative impact of elevating Joule heating phenomenon is noted on the molecular stabi
114 adient focusing (TGF) exploiting an inherent Joule heating phenomenon.
115                                Here, a flash Joule heating process is developed for ultrafast synthes
116 e sorbent's conductive nature permits direct Joule heating regeneration(2,3) using renewable electric
117 er above to facilitate air vibration through Joule heat release.
118                      The prevailing model of Joule heating relies on a simple semiclassical picture i
119                                   Minimizing Joule heating remains an important goal in the design of
120    The ultrafine nanoseeds achieved by rapid Joule heating render uniform deposition of Li metal anod
121                   It has been suggested that joule heating resulting from the applied pulse may play
122 turbances (LSTID) generated by high-latitude Joule heating seeded the instability soon after sunset.
123                                       First, Joule heating substantially impacts analytical sensitivi
124 arbon, which diffuses through the walls of a Joule-heated tantalum tube filled with graphite powder.
125 ted in parallel, resulting in a reduction of joule heating temperatures from 96.2 to 32.6 degrees C.
126                                          The Joule heating that contributes significantly to the heat
127 n-dissipative effects unlike plasmon induced Joule heating that occurs under resonance conditions.
128 n resistive heater as the thermal trigger of Joule heating, the device is able to on-demand destruct.
129 ing a transient FM state via current-induced Joule heating, the spin-orbit torque can switch the AFM
130                                         Upon Joule heating, the vertical device undergoes switching f
131 he liquid metal couples geometric changes to Joule heating, thus enabling tunable thermo-mechanochrom
132 ized particles in reduced graphene oxide are Joule heated to high temperature ( approximately 1,700 K
133                            By applying flash Joule heating to alpha-spodumene under an atmosphere of
134                       We apply just 5 min of Joule heating to promote the phase transition of the nan
135                                              Joule heating was not significant under the conditions t
136 of 645 V could be applied before significant Joule heating was observed.
137 l predictions of separation resolution (with Joule heating), we empirically demonstrate nearly fully
138 ion of intense electric fields and localized Joule heating, which are both highly confined to the fil
139 net generates a magnetic field and generates Joule heating, which can cause overheating.
140 rises from pure adiabatic currents devoid of Joule heating, while being a bulk effect not carried by
141 n-containing species by cost-effective flash Joule heating with a low energy input of 7.2 kJ per gram
142                      An experiment combining Joule heating with external heating/cooling further supp
143 ture of the substrate, we observe negligible Joule heating within the nanotube lattice itself and ins
144 creases, indicating the onset of traditional Joule heating within the nanotube.
145                        Urban mining by flash Joule heating would be 80x to 500x less energy consumpti

 
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