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Online since: October 2008
Authors: Luis Maria Esquivias Fedriani, Nicolás de la Rosa-Fox, Victor Morales-Flórez, Manuel Piñero
Table 1.
The upward curvature 0,0 0,1 0,2 0,3 0,4 0 10 20 30 (MPa) (%) 1 2 3 1,76 1,77 1,78 1,79 1,80 1,81 1,82 1,83 1,84 1 2 3 1,93 1,94 log [Er(t) (MPa)] log [t(s)] indicates a continuous increase in its elastic modulus, which is characteristic of elastomers that loose their stiffness as the polymer chains deform.
Nanoparticle Res., 1, 1 (1999)
Rev. 1, 243 (1994)
Soc (London) A319, 479 (1970) [56] J.
The upward curvature 0,0 0,1 0,2 0,3 0,4 0 10 20 30 (MPa) (%) 1 2 3 1,76 1,77 1,78 1,79 1,80 1,81 1,82 1,83 1,84 1 2 3 1,93 1,94 log [Er(t) (MPa)] log [t(s)] indicates a continuous increase in its elastic modulus, which is characteristic of elastomers that loose their stiffness as the polymer chains deform.
Nanoparticle Res., 1, 1 (1999)
Rev. 1, 243 (1994)
Soc (London) A319, 479 (1970) [56] J.
Online since: June 2016
Authors: Bernardo Buonomo, Oronzio Manca, Sergio Nardini, D. Ricci
This behaviour is more evident at low Peclet number values and Rayleigh number ones.
1.
Figure 1 – Scheme of a confined jet, impinging on a target surface.
a) b) Figure 14 - Local Nusselt number for fluid phase for Pe = 2000 and for: a) Ra = 400, f = 0%, 1% and 4%; b) f = 1% and Ra = 100, 200 and 400.
p particle s solid sf solid-fluid References [1] S.
Hung (1994), Impingement Cooling of an Isothermally Heated Surface with a Confined Slot Jet, ASME Journal of Heat Transfer 116, pp. 479–482
Figure 1 – Scheme of a confined jet, impinging on a target surface.
a) b) Figure 14 - Local Nusselt number for fluid phase for Pe = 2000 and for: a) Ra = 400, f = 0%, 1% and 4%; b) f = 1% and Ra = 100, 200 and 400.
p particle s solid sf solid-fluid References [1] S.
Hung (1994), Impingement Cooling of an Isothermally Heated Surface with a Confined Slot Jet, ASME Journal of Heat Transfer 116, pp. 479–482
Online since: December 2025
Authors: Elvin Y. Malikov, Seadet Humbetova, Samira Mammadova, Shamo Tapdiqov, Dilgam Taghiyev, Jamila Guliyeva, Ayaz Gulamirov
Fig. 1.
References [1] M.
Sci., vol. 3, no.1, pp.1–22, 2021, doi: 10.1016/j.nanoms.2020.12.002
Mater., vol. 43, pp. 469–479, 2013, doi: 10.1016/j.conbuildmat.2013.02.043
Mater., vol. 51, no. 1, pp. 10–16, 2021.
References [1] M.
Sci., vol. 3, no.1, pp.1–22, 2021, doi: 10.1016/j.nanoms.2020.12.002
Mater., vol. 43, pp. 469–479, 2013, doi: 10.1016/j.conbuildmat.2013.02.043
Mater., vol. 51, no. 1, pp. 10–16, 2021.
Online since: May 2022
Authors: Ambrose Njepu, S. Oladayo Oladejo, Gbenga Daniel Obikoya, Kayode Timothy Akindeji, Ibrahim Adeyanju, Adeniyi K. Onaolapo, Gulshan Sharma, Temitope Adefarati
The South African’ power generation capacity is currently dominated by coal-based power stations as shown in Fig. 1.
The technical specifications of each one of the components required for the simulation are presented in Table 1.
This indicates that a grid-connected HRES with the vertical axis tracking system is more economically feasible when compared with case study 1.
References [1] T.
Manag. vol. 105 (2015) 471–479
The technical specifications of each one of the components required for the simulation are presented in Table 1.
This indicates that a grid-connected HRES with the vertical axis tracking system is more economically feasible when compared with case study 1.
References [1] T.
Manag. vol. 105 (2015) 471–479
Online since: October 2010
Authors: Heinz Palkowski, Nicole Schulze, Mehdi Asadi
Accordingly, the thermal profile, as a function of time, has been determined for different values of z at y = 0 using measures of absorptivity, conductivity, specific heat and density of the present alloy of 0.57, 36.3 J m-1 s-1 K-1, 452 J kg-1 K-1 and 7840 kg m-3, respectively [57-59].
The EB powers were varied from 0.6 kW and 0.8 kW to 1 kW.
References [1] T.B.
Forum, Vol. 475-479 (2005), pp. 97-100 [39] P.C.M.
Tekkaya: Steel Research Int. 71 (2000), pp. 1-14
The EB powers were varied from 0.6 kW and 0.8 kW to 1 kW.
References [1] T.B.
Forum, Vol. 475-479 (2005), pp. 97-100 [39] P.C.M.
Tekkaya: Steel Research Int. 71 (2000), pp. 1-14
Online since: August 2015
Authors: Tadeusz A. Przylibski
Fig. 1.
Table 1.
Official Journal of the European Union, 17.1.2014., L 13/1 – L 13/73
Przylibski, Estimating the radon emanation coefficient from crystalline rocks into groundwater, Applied Radiation and Isotopes 53 (3) (2000) 473-479
Third edition incorporating the first and second addenda, Vol. 1, Recommendations.
Table 1.
Official Journal of the European Union, 17.1.2014., L 13/1 – L 13/73
Przylibski, Estimating the radon emanation coefficient from crystalline rocks into groundwater, Applied Radiation and Isotopes 53 (3) (2000) 473-479
Third edition incorporating the first and second addenda, Vol. 1, Recommendations.
Online since: May 2016
Authors: Rakshit Ameta, Surbhi Benjamin, Suresh C. Ameta, Dipti Soni, Neelu Chouhan
Fig. 1.
This system showed H2 generation rates of ∼434.29 ± 27.40 μmol h−1 g−1 under UV/Visible irradiation.
References [1] S.
Lee, Highly electrocatalytic Cu2ZnSn(S1–xSex)4 counter electrodes for quantum-dot-sensitized solar cells,ACS Applied Materials & Interfaces. 5(3) (2013) 479–484
Sun, Ultrasmall colloidal PbS quantum dots, Materials Chemistry and Physics. 147(1–2) (2014) 1–4
This system showed H2 generation rates of ∼434.29 ± 27.40 μmol h−1 g−1 under UV/Visible irradiation.
References [1] S.
Lee, Highly electrocatalytic Cu2ZnSn(S1–xSex)4 counter electrodes for quantum-dot-sensitized solar cells,ACS Applied Materials & Interfaces. 5(3) (2013) 479–484
Sun, Ultrasmall colloidal PbS quantum dots, Materials Chemistry and Physics. 147(1–2) (2014) 1–4