<p>The effects of the vacancy-type defects in the graphene sheet (GR) and volume fraction (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12221_2024_824_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{v}}_{\text{f}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>v</mtext> <mtext>f</mtext> </msub> </math></EquationSource> </InlineEquation>) of the GR on Young’s and shear moduli of polylactic acid (PLA) nanocomposite strengthened by the GR (GR/PLA) are investigated. The molecular dynamic (MD) method is implemented and stress–strain evolutions are extracted to explore elastic constants. The simulations demonstrate that adding the defect-free and defective GR in the PLA leads to a vast improvement in tensile and shear moduli. In every <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12221_2024_824_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{v}}_{\text{f}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>v</mtext> <mtext>f</mtext> </msub> </math></EquationSource> </InlineEquation> of the GR, the defective GR/PLA under tensile loadings compared to the defect-free one can endure smaller stress and deformation at the breaking point. Likewise, the bearable stress of the defective GR/PLA subjected to longitudinal shearing is lower than the maximum stress obtained from the defect-free GR/PLA. In any <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12221_2024_824_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{v}}_{\text{f}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>v</mtext> <mtext>f</mtext> </msub> </math></EquationSource> </InlineEquation> of the GR, as the rate of the defects rises, the defective GR/PLA is capable of withstanding a smaller quantity of ultimate stress. However, the variation of the ultimate deformation of defective nanocomposites with the increase of the defect content does not pursue a determined trend, mainly because it is heavily dependent on the distribution pattern and location of defects. Young’s and shear moduli of the GR/PLA experience a downward trend with increasing the degree of the defect. In a desired defect percentage, the stiffness and rigidity of the nanocomposites become larger by choosing a higher GR’s <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12221_2024_824_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{v}}_{\text{f}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>v</mtext> <mtext>f</mtext> </msub> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Mechanical Properties of Defective Graphene-Reinforced Polymer Nanocomposite: A Molecular Dynamics Simulation Study

  • S. Haghighi,
  • Y. Keramati,
  • M. Eghbalian,
  • R. Ansari

摘要

The effects of the vacancy-type defects in the graphene sheet (GR) and volume fraction ( \({\text{v}}_{\text{f}}\) v f ) of the GR on Young’s and shear moduli of polylactic acid (PLA) nanocomposite strengthened by the GR (GR/PLA) are investigated. The molecular dynamic (MD) method is implemented and stress–strain evolutions are extracted to explore elastic constants. The simulations demonstrate that adding the defect-free and defective GR in the PLA leads to a vast improvement in tensile and shear moduli. In every \({\text{v}}_{\text{f}}\) v f of the GR, the defective GR/PLA under tensile loadings compared to the defect-free one can endure smaller stress and deformation at the breaking point. Likewise, the bearable stress of the defective GR/PLA subjected to longitudinal shearing is lower than the maximum stress obtained from the defect-free GR/PLA. In any \({\text{v}}_{\text{f}}\) v f of the GR, as the rate of the defects rises, the defective GR/PLA is capable of withstanding a smaller quantity of ultimate stress. However, the variation of the ultimate deformation of defective nanocomposites with the increase of the defect content does not pursue a determined trend, mainly because it is heavily dependent on the distribution pattern and location of defects. Young’s and shear moduli of the GR/PLA experience a downward trend with increasing the degree of the defect. In a desired defect percentage, the stiffness and rigidity of the nanocomposites become larger by choosing a higher GR’s \({\text{v}}_{\text{f}}\) v f .