2022
DOI: 10.1002/mame.202200424
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Enhancement on Thermal and Mechanical Properties of Insulating Paper Cellulose Modified by Silane Coupling Agent Grafted hBN

Abstract: The performance of insulating paper cellulose is an important factor affecting the normal operation of electric power equipment. This paper uses molecular dynamics methods to establish pure cellulose, hBN‐modified cellulose, 3‐aminopropyltriethoxysilane (KH550), 3‐glyoxypropyltrimethoxysilane (KH560), and 3‐methylpropoxypropyltris (KH570) grafted with hBN modified cellulose models. The effect of cohesive energy density (CED), thermal conductivity (TC), mean square displacement (MSD), free volume, glass transit… Show more

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Cited by 13 publications
(9 citation statements)
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References 34 publications
(52 reference statements)
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“…The amorphous region of cellulose selected for this paper belongs to the glassy state, and the mutation from the glassy state to the highly elastic state occurs as the temperature increases, and this abrupt change point temperature is also the glass transition temperature 32 . In this paper, the glass transition temperature of each model is measured by specific volume‐temperature curve method 31 . The model is continuously warmed up from 303 K to 703 K by molecular dynamics to obtain an image of the change in model specific volume versus temperature, and the mutation point can be found by curve fitting on this image, and this mutation point is the glass transition temperature, and the results are shown in Figure 4.…”
Section: Resultsmentioning
confidence: 99%
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“…The amorphous region of cellulose selected for this paper belongs to the glassy state, and the mutation from the glassy state to the highly elastic state occurs as the temperature increases, and this abrupt change point temperature is also the glass transition temperature 32 . In this paper, the glass transition temperature of each model is measured by specific volume‐temperature curve method 31 . The model is continuously warmed up from 303 K to 703 K by molecular dynamics to obtain an image of the change in model specific volume versus temperature, and the mutation point can be found by curve fitting on this image, and this mutation point is the glass transition temperature, and the results are shown in Figure 4.…”
Section: Resultsmentioning
confidence: 99%
“…The glass transition temperature is the temperature corresponding to the point of abrupt change in the physical properties such as mechanical, thermodynamic, electromagnetic, deformation, and optical properties of the polymer. 31 The amorphous region of cellulose selected for this paper belongs to the glassy state, and the mutation from the glassy state to the highly elastic state occurs as the temperature increases, and this abrupt change point temperature is also the glass transition temperature. 32 In this paper, the glass transition temperature of each model is measured by specific volume-temperature curve method.…”
Section: Glass Transition Temperaturementioning
confidence: 99%
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“…The mechanical properties can be characterized by the stress–strain curve and mechanical parameters such as the elastic modulus ( E ), the bulk modulus ( K ), and the shear modulus ( G ). According to the Hooke's law, applying stresses along the model x – x , y – y , z – z , x – y , y – z , and z – x directions, respectively, the model will generate the corresponding strains, and the stress–strain relationship meets the following equation [ 44 ] [σ1σ2σ3σ4σ5σ6]=[C11C21C31C41C51C61C12C22C32C42C52C62C13C23C33C43C53C63C14C24C34C44C54C64C15C25C35C45C55C65C16C26C36C46C56C66]·[ε1…”
Section: Resultsmentioning
confidence: 99%
“…The FVF is a ratio of free volume (Vf$V_{\text{f}}$) to total volume (Vt$V_{\text{t}}$) in the model. [ 19,44,46 ] The free volume theory suggests that the total volume of the polymer materials is composed of free volume and occupied volume (Vo$V_{\text{o}}$). The FVF can be expressed asFVF=VfVf+Vo$$\text{FVF} = \frac{V_{\text{f}}}{V_{\text{f}} + V_{\text{o}}}$$…”
Section: Resultsmentioning
confidence: 99%