2015
DOI: 10.1016/j.rser.2014.08.087
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Thermal transmittance of carbon nanotube networks: Guidelines for novel thermal storage systems and polymeric material of thermal interest

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Cited by 36 publications
(26 citation statements)
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“…The impact of horizontal overlap, a, is simulated in the range 20-80 Å, with b fixed at 0 Å, h at 4 Å and angular displacement set to θ = (0,0,0). As depicted in Figure 3a and previously reported [36], R k decreases with larger horizontal overlap following a power law, because this allows enhanced van der Waals interactions between GNRs and thus better phononic heat transfer [44]. A similar behaviour is observed for varying values of vertical overlap (b tested in the range 0-18 Å, with a fixed at 40 Å, h at 4 Å and θ = (0,0,0)), since less overlapping area (i.e., higher b) leads to a power increase of R k (see Figure 3b).…”
Section: Resultssupporting
confidence: 73%
See 1 more Smart Citation
“…The impact of horizontal overlap, a, is simulated in the range 20-80 Å, with b fixed at 0 Å, h at 4 Å and angular displacement set to θ = (0,0,0). As depicted in Figure 3a and previously reported [36], R k decreases with larger horizontal overlap following a power law, because this allows enhanced van der Waals interactions between GNRs and thus better phononic heat transfer [44]. A similar behaviour is observed for varying values of vertical overlap (b tested in the range 0-18 Å, with a fixed at 40 Å, h at 4 Å and θ = (0,0,0)), since less overlapping area (i.e., higher b) leads to a power increase of R k (see Figure 3b).…”
Section: Resultssupporting
confidence: 73%
“…In fact, above the percolation threshold, R k at filler-filler interfaces has a fundamental role in determining the effective thermal conductivity of PNCs, since direct contact between contiguous fillers takes place [43]. Fasano et al have studied the effect of geometry and filler functionalization on the overall thermal transmittance of networks of carbon nanotube fillers [44]. In particular, they noticed that the thermal resistance at the filler-filler interface strongly decays with both the overlapping area and concentration of covalent cross-linkers between adjacent carbon nanotubes.…”
Section: Introductionmentioning
confidence: 99%
“…First, opposite trends are noticeable re-garding the relation between thermal conductivity and decreasing particle size: (1) a decrease of thermal conductivity because of the increase in the overall solid-liquid interface effects [45,[126][127][128][129][130][131] (Fig. 4); (2) an increase of thermal conductivity because of the nanolayer effect and the increase of random motion of nanoparticles, which promotes the creation of percolation paths [89,98,[132][133][134].…”
Section: Thermal Properties Of Nanofluidsmentioning
confidence: 99%
“…Later, Shen and coworkers 35 investigated the ITC in epoxy resin/graphene nanocomposites, as a function of the chemical functionalization of graphene, and showed that the highest ITC reduction occurs with triethylenetetramine moieties, because of their ability to penetrate in the epoxy resin and form covalent bonds. On the other hand, the thermal conductance associated with filler-filler contacts, in this work referred to as Thermal Boundary Conductance (TBC), was also studied numerically by various authors, specifically between carbon nanotubes and graphene platelets surface-functionalized with small bridging groups such as oxygen or methylene bridges [36][37][38][39] , short alkyl chains 40 or benzene 41 . TBC of alkyl molecular junctions covalently bound between two graphene flakes was investigated in details by Li and coworkers 40 Recently, we also reported NEMD simulations of edge-to-edge alkyl junctions between graphene nanoribbons 42 , where covalent bonding was compared to Van der Waals forces between interpenetrating molecules.…”
Section: Introductionmentioning
confidence: 99%