ライフサイエンスコーパス: Joule heat

1 ing-to-conducting phase transition driven by Joule heating.

2 at strains as high as 140%, and can support Joule heating.

3 the sensor recovery time, probably by local Joule heating.

4 e atomic scale, for graphitic nanoribbons by Joule heating.

5 ot cause significant intra- or extracellular Joule heating.

6 rmometer, we mapped the thermal expansion of Joule-heated, 80-nanometer-thick aluminum wires by preci

7 rbed RF energy in brain tissue converts into Joule heat and affects the nuclear magnetic shielding an

8 During Joule heating and electron beam irradiation, carbon atom

9 Paper based ITP is challenged by Joule heating and evaporation because it is open to the

10 t of electroporation protocols that minimize Joule heating and maximize cell viability.

11 In this study, we investigated Joule heating and pH as parameters controlling the dewat

12 constructive interference effect between the Joule heating and temperature-dependent resistance effec

13 Electromagnetic mechanism of Joule heating and thermal conduction on conductive mater

14 surface electrodes for actuation, localized Joule heating, and thermistic temperature sensing.

15 0.1 MV.cm(-1), indicating that effects from Joule heating are minor.

16 temperature gradients resulting from intense Joule heating at constrictions between grains.

17 Additionally, Joule heating can potentially induce thermal flow and mo

18 flux and the responding electric energy, the Joule heating, consumed in the cell membrane, as well as

19 periment are a critical aspect in iDEP since Joule heating could lead to various detrimental effects

20 nm, allowing us to identify the presence of Joule heating, current crowding and thermoelectric heati

21 Both electrical current and Joule heating diminish with increasing pressure, and the

22 Joule heating effects are expected to be acute in open m

23 In addition, a model of Joule heating effects in the microdevice during operatio

24 By a comparison with the shock field-induced Joule heating effects on cell membranes, the field-induc

25 film carbon nanotube (CNT)/polymer composite Joule heating element can prevent CNT degradation in ion

26 We develop numerical simulations of Joule heating-enhanced diffusion during electrophoresis

27 perature-controlled electrodes revealed that Joule heating enhances water removal by increasing evapo

28 intrinsically affected by the generation of Joule heating, entailing a drop in viscosity and possibl

29 f attolitres (10(2)-10(5) nm3) of polymer by Joule heating, extremely non-uniform electric field grad

30 ted effects such as transverse diffusion and Joule heating for a given faceted prism.

31 The attractive advantages of Joule-heat-free transmission of information, utilization

32 In the former, controlled Joule heating generated by a voltage-biased quantum poin

33 ing temperature distributions resulting from Joule heating in a variety of microfluidic circuits that

34 trogen species through high-power electrical joule heating in ammonia gas, leading to n-type electron

35 It generates sound thermoacoustically by Joule heating in graphene.

36 locally up to 1000 K, validating the role of Joule heating in resistive switching.

37 ts were attributed to less gas formation and Joule heating in SFE.

38 Joule-heating induced conductance-switching is studied i

39 n of suspended few-layer graphene by in situ Joule-heating inside a transmission electron microscope.

40 alyte diffusivity due to autothermal runaway Joule heating is a dominant mechanism that reduces separ

41 gh as 600 V/cm could be applied with minimal Joule heating (<2 degrees C).

42 This heat can be generated via a Joule heating mechanism or high power laser pulses.

43 les, which are synthesized via a novel rapid Joule heating method, can serve as nanoseeds to direct t

44 By optimizing the Joule heating method, ultrafine Ag nanoparticles ( appro

45 y in the crossover channel indicates that no Joule heating occurs at voltages of at least 2.0 kV.

46 tron thermal microscopy to detect the remote Joule heating of a silicon nitride substrate by a single

47 plications in nanoscale electronics, because Joule heating of interconnecting wires is a major proble

48 ectrically induced actuation associated with Joule heating of the matrix when a current is passed thr

49 adient focusing (TGF) exploiting an inherent Joule heating phenomenon.

50 The prevailing model of Joule heating relies on a simple semiclassical picture i

51 Minimizing Joule heating remains an important goal in the design of

52 The ultrafine nanoseeds achieved by rapid Joule heating render uniform deposition of Li metal anod

53 It has been suggested that joule heating resulting from the applied pulse may play

54 First, Joule heating substantially impacts analytical sensitivi

55 arbon, which diffuses through the walls of a Joule-heated tantalum tube filled with graphite powder.

56 n-dissipative effects unlike plasmon induced Joule heating that occurs under resonance conditions.

57 n resistive heater as the thermal trigger of Joule heating, the device is able to on-demand destruct.

58 ized particles in reduced graphene oxide are Joule heated to high temperature ( approximately 1,700 K

59 Joule heating was not significant under the conditions t

60 of 645 V could be applied before significant Joule heating was observed.

61 l predictions of separation resolution (with Joule heating), we empirically demonstrate nearly fully

62 An experiment combining Joule heating with external heating/cooling further supp