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In a letter in 1962, Pope et al. [3] demonstrated faint electroluminescence from anthracene crystals, 10-20 mm thick.
The cathode is a Ca layer protected by another Al coating, both thermally evaporated.
The electroluminescence (EL) follows PL exactly with respect to the main peak.
Hence origin of luminescence in EL is the same as in PL.
But, interestingly, PS-4 shows an additional broad EL spectrum which is white in color coordinates.

It was found that in Al and Cu dispersion strengthened systems a trajectory of the fracture changes at about 8-12 wt. % fraction of the secondary phase [17, 18].
El-Morsy, A.
Ivan, Failure mechanism of dispersion strengthened Al-Al4C3 systems, J. of Mater.
Gobin, A study of damage under tensile loading in a new Al-Si-Fe alloy processed by the Osprey route, Mater.
Krock, Analysis of deformation of Al-Si system, Compos.

Puska et al.[4] have calculated the lifetime values of GaSb bulk and obtained a value of 257ps.
Ling et al. [7] have observed positron shallow trapping in positron lifetime study on Zn-doped GaSb, and found the shallow trap was ionized dopant acceptor Zn.
GaSb is an acceptor-type defect in GaSb, and Hu el al. [8] have found this kind of antisite defect acts as positron shallow trap in undoped GaSb.
Beling, et al: Phys Rev B Vol. 64 (2001), p. 075201
Su, et al: Physics Letters A Vol. 332 (2004), p. 286.

Effect of Annealing Temperature Variation on Al-Doped Nickel Oxide Thin-Film Synthesized by Dip-Coating Technique S.
Aluminum nitrate (Al (NO3)3) was used as a dopant.
SEM investigation SEM was used to examine the top portion morphology of the Al-doped NiO films that were laid on a glass surface.
Binas ,Highly sensitive and selective NO2 chemical sensors based on Al doped NiO thin films. 
El Whibi, E.Tessarolo, M.Rigon,A.

Cai, et al., Nonlinear analysis of 3-D seismic interaction of soil-pile-structure systems and application, Eng.
Maheshwari, et al., Gould, Three-dimensional finite element nonlinear dynamic analysis of pile groups for lateral transient and seismic excitations, Can.Geotech.
[6] M.El-Attar, et al., Non-linear cable response to multiple support periodic excitations.

Synthesis of Iron Oxide Nanowires by Heating Iron Foils Hyoun Woo Kim 1,a, Seung Hyun Shim 1,b, Beom Hoan O2,c, Seung Gol Lee 2,d, Se-Geun Park2,e and El-Hang Lee2,f 1 School of materials science and engineering, college of engineering, Inha University, 253 Yong Hyun Dong, Nam Gu, Incheon 402-751, Republic of Korea 2 OPERA, Micro-Photonics Advanced Research Center (µ-PARC), School of Information and Communication Engineering, INHA University, 253 Yong-hyun-dong, Nam-gu, Incheon 402 751, Republic of Korea a hwkim@inha.ac.kr, bshimseun@naver.com, cobh@inha.ac.kr, dsglee@inha.ac.kr, e sgpark@inha.ac.kr, fehlee@inha.ac.kr Keywords: Thermal evaporation, Iron oxide, Nanowires.
However, not many work exists for nanoscale iron oxide and Lian et al. reported the synthesis of Fe3O4 nanorods in a solution-phase approach [13].
Lee et al. [18] and the report of B.
Kim et al. on the preparation of Ga2O3 nanomaterials (nanowires) from GaN powders in a N2 atmosphere [19].

The base of the dissipation calculation is the electrical efficiency ηel, that is used to calculate the electrical power loss PL,el of the motor.
PL,Cu,R = PRF · s (2) PL,R ≈ Pin · s (3) PL,S = PL,el − PL,R (4) Bearing friction torque (heat source).
Abele et al., Machine tool spindle units, in: CIRP Annals - Manufacturing Technology 59 (2010), pp. 781-802
Chen et al., Thermal error of a hydrostatic spindle, Precision Engineering 35 (2011), pp. 512-520
Kempkes et al., Elektrotechnik und Elektronik für Maschinenbauer, second ed., Springer, Berlin Heidelberg, 2012

Fenner, et al, Science, 313 (2006) 1072
Fraysse, et al, Water Science and Technology, 50 (2004) 23
El-Din, Ozone Science & Engineering, 28 (2006) 353
Bauer et al, Journal of Environment Management, 79 (2006) 215 [7] S.
Krause, et al, Journal of Hazardous Materials, 149 (2007) 631

Attia et al [3] introduces a numerical model for the analysis of contact problems of nonlinear thermal viscoelastic viscoplastic bodies, whose viscoelastic behavior belongs to a class of thermal rheologically complex materials.
Brackbill et al [4] proposed a thermomechanical model for elastomeric materials using the method of anelastic displacement fields.
A thermo-visco-hyperelastic constitutive model, in accordance with the second thermodynamics principle, is formulated to describe the self-heating evolution in elastomeric materials under cyclic loading by Ovalle Rodas et al [5].
It can be noticed that the computed temperature is overestimated, similar to the studies by Boukamel et al [10].
[3] M A Attia, A G El-Shafei and F F Mahmoud: Int J Eng Sci Vol.78 (2014), p. 1

Tensile properties and HER of PO/HGI 780CP steels Steels YS, MPa UTS, MPa YE, % T-El, % HER, % Uncoated 780CP 697 798 - 18 61 Coated 780CP 742 795 1.1 17 72 Fig. 3.
[2] Zhong, N., et al.
[3] Ohjoon, K. et al.
) [4] De Cooman, B. et al., Mat.
Tech. 28(2012), pp.513-527 [5] TAYLOR, Mark D., et al.