Convection Heat Transfer

By R. Lewis, Perumal Nithiarasu, K. N. Seetharamu. 2005

1,209 citations recorded by the source corpus.

Subfields: Computational Mechanics, Mechanical Engineering

View Paper: https://www.semanticscholar.org/paper/8df8b64b3a4eaca70676c296044c16362dbc25c7

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In Computational Mechanics

In Mechanical Engineering

Citations in the corpus

Heatline analysis on natural convection for nanofluids confined within square cavities with various thermal boundary conditions (2012, background): “Heatline concept was developed by earlier researchers [37,38] to visualize conductive as well as convective heat transport.”
Three-dimensional analysis of heat transfer in a micro-heat sink with single phase flow (2004, positive): “As indicated by Bejan [14], the following approximation yields reasonably approximate results for this type of problem,”
Enhancement of external forced convection by ionic wind (2008, neutral): “The forced convection component here includes both the bulk flow and ionic wind components, while the free convection value was estimated using the correlation [31]”
Computational Fluid Dynamics for urban physics: Importance, scales, possibilities, limitations and ten tips and tricks towards accurate and reliable simulations (2015, methodology): “Note that for including the effect of density differences due to temperature or species concentrations, generally the Boussinesq approximation for buoyancy is applied [179].”
Particle Penetration Through Building Cracks (2003, methodology): “We used scale analysis (Bejan 1984) to estimate the particle concentration boundary layer thickness within the crack.”
Solar evaporation enhancement using floating light-absorbing magnetic particles (2011, background): “@ θ = 0: Tsw = Tsw sat (5) @ z = 0, any θ > 0: −Ksw ∂Tsw ∂z = 𝑕sw 1 − φ (Ts − Tsw ) (6) @ z = lsw , any θ > 0: ∂Tsw ∂z = 0 (7)”
Active cooling by metallic sandwich structures with periodic cores (2005, background): “The Nusselt number is independent on the Reynolds number in the laminar regime (Nuh 4, depending slightly on the cross-section geometry), whereas for turbulent flow [27]: Nuh 1⁄4 ðfh=8ÞðReh 1000ÞPr 1 þ 12.”
Soret effect on mixed convection flow in a nanofluid under convective boundary condition (2013, background): “A detailed review of mixed convective heat and mass transfer can be found in the book by Bejan [7].”
Effective thermal conductivity of rough spherical packed beds (2006, background): “Also, natural convection does not occur within the gap between particles when the Grashof number is less than 2500 [11].”
Fluid flow and heat transfer of non-Newtonian nanofluid in a microtube considering slip velocity and temperature jump boundary conditions (2017, background): “of the nanofluid raises due to increased heat conduction coefficient; However the thermal entrance length can be determined by Lt = CtD Re Pr which Ct is the thermal entrance length coefficient [53,54].”
Conduction and entrance effects on laminar liquid flow and heat transfer in rectangular microchannels (2005, methodology): “The model used the conventional mass, momentum and energy equations [21].”