2022
DOI: 10.1021/acs.energyfuels.1c04140
|View full text |Cite
|
Sign up to set email alerts
|

Metal Oxide Nanoparticle Dispersed-Polyethylene Glycol: Thermal Conductivity and Thermal Energy Storage Properties

Abstract: Polyethylene glycols as phase change materials (PCMs) have good latent heat storage (LHS) characteristics, but the low thermal conductivity property significantly hinders their usage potential in thermal energy storage (TES) applications. Within this framework, four different metal oxide nanoparticles (Al2O3, CuO, TiO2, and ZnO) dispersed-PEG as thermal conductivity enhanced PCMs were developed for TES purposes. Sediment photographs and scanning electron microscopy/energy dispersive spectroscopy (SEM/EDX) anal… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

2023
2023
2024
2024

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 7 publications
(2 citation statements)
references
References 62 publications
0
2
0
Order By: Relevance
“…However, the contribution of these vibrational modes to heat transfer is still unclear. To deeply analyze the relative contributions from different vibrational modes to the total thermal conductivity, the spectral contributions to the heat flux (q(ω)) is calculated, which is defined as 42,43…”
Section: Simulation Model and Detailsmentioning
confidence: 99%
See 1 more Smart Citation
“…However, the contribution of these vibrational modes to heat transfer is still unclear. To deeply analyze the relative contributions from different vibrational modes to the total thermal conductivity, the spectral contributions to the heat flux (q(ω)) is calculated, which is defined as 42,43…”
Section: Simulation Model and Detailsmentioning
confidence: 99%
“…However, the contribution of these vibrational modes to heat transfer is still unclear. To deeply analyze the relative contributions from different vibrational modes to the total thermal conductivity, the spectral contributions to the heat flux ( q (ω)) is calculated, which is defined as , q 1 J ( ω ) = 2 italicAM normalΔ t j J i I false⟨ i J ( ω ) · i false( ω false) * false⟩ where F̃ i and ṽ i are the Fourier transforms of force and velocity vectors, respectively; A denotes the surface area; Δ t is the time interval between two continuous configurations; and M is the number of configurations. Here, atomic forces and velocities are saved every 5 fs for a total of 3 ns.…”
Section: Simulation Model and Detailsmentioning
confidence: 99%