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Online since: July 2013
Authors: Jennifer Keenahan, Ciaran H. Carey, Eugene J. O'Brien
Law et al. [6] and Yu & Chan [7] later use a frequency time domain method, in which a Fourier transform is performed on the equation of motion and the force histories are found directly using the least squares method.
Law et al. [9] use a finite element method to identify the axle loads and a condensation technique to reduce the system to a smaller number of master degrees of freedom.
The damage is modelled as recommended by Sinha et al
El-Osery, and M.
Online since: February 2013
Authors: Zhen Hua Liu, Ying Shi Zhao, Yue Ming Hu
According to soil thermal characteristic, the thermal inertia model was firstly developed and applied in the geologic interpretation using infrared (IR) images by Watson et al[1].
Zhang et al. [13] proposed a thermal inertia model considering surface sensible and latent fluxes, but neglecting vegetation and soil two-layer impact, and derive soil moisture availability by differential thermal inertia, after many experiments, only using remotely sensed information rather than local soil parameters such as soil properties and type.
XUE and et al[14] developed a thermal inertia model to be suitable in situations whether or not the satellite overpass time coincides with the local maximum and mini-mum temperature time.
[5]SOBRINO, J.A., and KHARRAZ, M.H.El., Combining afternoon and morning NOAA satellites for thermal inertia estimation 2, Methodology and application, Journal of Geophysical Research.
Online since: September 2014
Authors: Guo Cai Zhou, Hai Qing Pei
[3] Matlik JF, Farris TN, Haake FK, et al.
[6] Hirschberger CB, Peerlings RHJ, Brekelmans WAM, et al.
Mod-elling Simul.
[10] Yin ZY, Yue ZF, Yang ZG, et al.
Online since: June 2018
Authors: Selim Gürgen
Lee et al. [3] studied the deformation modes of polyethylene based high performance fabrics in multi-layer targets.
Chu et al. studied the impact resistance of aramid based fabrics at oblique impact conditions changing the weave types of fabrics.
To show the influence of composite laminate thickness, Gellert et al. [9] investigated targets with various thicknesses under ballistic impacts.
El-Shiekh, An Experimental Investigation of High Velocity Impact and Penetration Failure Modes in Textile Composites, J.
Online since: October 2012
Authors: Hui Zhou, Ping Hu
Second is the destructive position of the faceplate, the destructive position is affected by V shape valley, U shape valley, the ratio of width and height, the wave spread direction et al.
Zhang et al. studied the seismic coefficient of earth-rockfill dams higher than 150m.
Table 1 The computational cases Wave Seismic intensity Height of the dam(m) Width of the valley(m) Slope ratio of the bank (1) Taft wave (2) El Centro wave (3) Banshen wave (4) Shenhu wave (1) 7° (2) 8° (3) 9° (1) 100 (2) 150 (3) 200 (4) 250 (5) 300 (1) 50 (2) 150 (3) 300 (4) 500 (1) 0.4 (2) 0.6 (3) 0.8 (4) 1.0 (5) 1.5 The crest width of the dam is 10m, the slope ratios of the upstream and downstream are 1:1.6, the density of the rockfill is and the density of the concrete faceplate is .
[10] KONG Xian-jing, LOU Shu-lian, ZOU De-gao, et al.
Online since: January 2004
Authors: P.A. Sterne, Amy L.R. Bug, Melaku Muluneh, Jillian Waldman
For comparison, we have also calculated the lifetimes in a finitetemperature version of the PIB model by summing the appropriate Bessel function contributions for the given sphere size and temperature, following Goworek et al.[5].
We are also able to study mesopores at finite temperature, as suggested by Gidley et al.[5] for application to thin films.
While this model might be embellished to include polarization, Si and Al, counterions and adsorbates; it provides a starting point from which to consider various cage structures.
[3] E.L.
Online since: November 2016
Authors: Marcos Flavio de Campos, Daniel Rodrigues
Honda et al [16] suggested the following expression, Eq. (8) for copper losses, where A and B are experimental constants, and the GAP-corrected permeability mcorr as given by Eq. (9)
Liu et al [26] emphasize that MnBi is very sensitive to oxidation and is unstable above 473 K, making very difficult the processing.
El-Mansy, K.
Lantz et al.: IEEE Transactions on Magnetics, 2015.
Online since: August 2016
Authors: João Carlos Silos Moraes, Alailson Domingos dos Santos, Michela Melissa Duarte Seixas Sostena, José Carlos Barbosa, Paulo Henrique dos Santos, Maria Giovanna Gandolfi, Carlo Prati
The value obtained by us agrees better with that reported by Fidel, et al. [15].
Tagger, et al. [16] evaluated the adhesion of nine endodontic cements with different bases (epoxy resins, glass-ionomer, zinc oxide-eugenol and salicylate resins) and the results showed that the epoxy resin-based cements promote better adhesion.
Lee, et al. [17] suggest that the epoxy resin provides good adhesion between the dentin and the gutta-percha because it promotes chemical reactions with dentin substrates and gutta-percha.
Spano, E.L.
Online since: March 2019
Authors: Wai Lin, Ola Gawi, Quosay A. Ahmed, Mohammed Abdalla Ayoub, Anas Hasan, Mysara Eissa Mohyaldinn, Mokhtar Che Ismail
Olusegun et al [9] have tested Jatropha leaves extract for corrosion inhibitors and reported corrosion inhibition efficiency of 93.69%.
Abd-El-Nabey, and M.
[12] J., O.S., et al., Jatropha Curcas Leaves Extract as Corrosion Inhibitor for Mild Steel in 1M Hydrochloric Acid.
[15] O., M., et al., Inhibition of Steel Corrosion in 1M HCl by Jatropha Curcas oil.
Online since: August 2010
Authors: Shi Gang Wang, Bai Rui Tao, Hong Xia Zhang, Xi Bing Li
ρπ b b v vfg vee b WWWr d h Tkl Q , (6) The mathematical model of continuous flow limit of the circular micro heat pipe with a trapezium-grooved wick structure is   > ≤ =      = − molecules freeor thin of flow01.0 flow vapor continuous 01.0 6 2 051.1 3 2 A vv v n � M dp kT K πρπ (7) The mathematical model of frozen startup limit of the circular micro heat pipe with a trapezium-grooved structure is ( ) ( ) 1 2 ≥ − + ∞TTC hWWn mel fglb δρ (8) In Eq.(1)-(8), max,viQ -viscous limit of micro heat pipe (W); max,sQ -sonic limit of micro heat pipe (W); max,eQ -entrainment limit of micro heat pipe (W); max,caQ -capillary limit of micro heat pipe (W); max,coQ -condensing limit of micro heat pipe (W); max,bQ -boiling limit of micro heat pipe (W); effl -effective length of micro heat pipe (m); el
-evaporator length of micro heat pipe (m); cl -condenser length of micro heat pipe (m); al -adiabatic section length of micro heat pipe (m); l -total length of micro heat pipe (m); fgh -latent heat of evaporation of working fluid (J/kg); vρ -vapor density of working fluid (kg/m3); lρ-liquid density of working fluid (kg/m3); ρ-liquid density at the melting point of working fluid (kg/m3); vp -vapor saturation pressure of working fluid (Pa); vµ -vapor viscosity of working fluid (N·s/m2); lµ-liquid viscosity of working fluid (N·s/m2); σ-liquid surface tension of working fluid (N/m); vγ -specific heat ratio of vapor ( for one-atom vapor it is 5/3,for double-atom vapor it is 7/5,and for multiple-atom vapor it is 4/3); R0-universal gas constant (J/kmol·K); Tv:operating temperature of micro heat pipe (K); M-relative molecular mass of working fluid (g/mol); br -critical radius of bubble generation (m); W-top-width of trapezium groove (m); Wb-bottom-width of trapezium groove
[6] Launay S., Sartre V., Mantelli M.B.J., et al: Int.
[11] Nilson R.H., Tchikanda S.W., Griffiths S.K., et al: Int.
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