By Xinwei Wang
This e-book covers the recent applied sciences on micro/nanoscale thermal characterization constructed within the Micro/Nanoscale Thermal technological know-how Laboratory led via Dr. Xinwei Wang. 5 new non-contact and non-destructive applied sciences are brought: optical heating and electric sensing strategy, brief electro-thermal method, temporary photo-electro-thermal method, pulsed laser-assisted thermal leisure strategy, and steady-state electro-Raman-thermal process. those suggestions characteristic considerably greater ease of implementation, large signal-to-noise ratio, and feature the ability of measuring the thermal conductivity/diffusivity of varied one-dimensional constructions from dielectric, semiconductive, to steel materials.Content:
Chapter 1 advent (pages 1–46):
Chapter 2 Thermal Characterization in Frequency area (pages 47–86):
Chapter three brief applied sciences within the Time area (pages 87–140):
Chapter four Steady?State Thermal Characterization (pages 141–204):
Chapter five Steady?State Optical?Based Thermal Probing and Characterization (pages 205–246):
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Additional resources for Experimental Micro/Nanoscale Thermal Transport
1, which encompasses all the internal scattering effects, provided the material is homogeneous. 22 is an approximation that describes the average behavior of phonon transport, it sufﬁces to capture the essential physics of interest. In the LBM, an artiﬁcial lattice is attached to the space and the BTE is discretized by laying all particles at grid intersections and allowing them to move only along the linkages of nodes. This ﬁnite set of movements can well represent the real particle motion if the lattice pattern is properly chosen according to the nature of the transport process in question.
This will lead to a smaller thermal conductivity in the thickness direction than that in the in-plane direction as discussed later. For boundary scattering effect, the Matthiessen rule (10) relates the effective thermal relaxation time (τe ) to the thermal relaxation time in bulk materials (τ ) and the thermal relaxation time by pure boundary scattering (τb ) as follows: 1 1 1 = + . 47) For simple geometries, τb can be obtained with kinetics analysis. For complicated geometries, determining τb becomes a nontrivial work.
Gacek and X. Wang, Journal of Applied Physics 104 (12), 126101 (2008). S. Gacek and X. Wang, Applied Physics A 94 (3), 675–690 (2008). S. Gacek and X. Wang, Physics Letters A 373 (37), 3342–3349 (2009). L. Guo and X. Wang, Journal of Physics D: Applied Physics 42 (1), 015307 (2009). F. P. Incropera and D. P. DeWitt, Fundamentals of Heat and Mass Transfer, 5th ed. (John Wiley & Sons, New York, 2002). W. P. Mason, Acoustic Properties of Solids, 3rd ed. (McGraw-Hill, New York, 1972). S. V. J. Narumanchi, J.