<p>This study systematically investigates the separation performance of porous <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(Al_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>A</mi> <msub> <mi>l</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(O_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>O</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> for neon isotopes (<InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{20}Ne\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>20</mn> </mmultiscripts> <mi>N</mi> <mi>e</mi> </mrow> </math></EquationSource> </InlineEquation>/<InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{22}Ne\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>22</mn> </mmultiscripts> <mi>N</mi> <mi>e</mi> </mrow> </math></EquationSource> </InlineEquation>) under cryogenic conditions through molecular dynamics (MD) simulations. By constructing <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(Al_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>A</mi> <msub> <mi>l</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(O_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>O</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> models with varying pore sizes (4.5–15 Å) and performing MD simulations, the critical effects of pore size and temperature on separation factors are revealed. The results demonstrate that <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-<InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(Al_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>A</mi> <msub> <mi>l</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(O_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>O</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> with sub-6 Å&#xa0;pore size exhibits remarkable isotopic sieving capability under a fixed pore volume of 0.6 <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq18.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {cm}^3/\hbox {g}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mtext>cm</mtext> <mn>3</mn> </msup> <mo stretchy="false">/</mo> <mtext>g</mtext> </mrow> </math></EquationSource> </InlineEquation>. Specifically, the 4.5 Å&#xa0;pore-sized material achieves a separation factor of 1.333 at 30 K, indicating preferential kinetic selectivity for <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{20}Ne\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>20</mn> </mmultiscripts> <mi>N</mi> <mi>e</mi> </mrow> </math></EquationSource> </InlineEquation>. Reduced temperatures significantly enhance separation performance, provided that the pore size is sub-10 Å. The diffusion coefficient’s dependence on both temperature and pore diameter follows the Knudsen diffusion mechanism. This research establishes that microporous <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-<InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(Al_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>A</mi> <msub> <mi>l</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10967_2025_10222_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(O_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>O</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> enables effective neon isotope separation through combined molecular sieving and kinetic discrimination effects, offering theoretical foundations for developing advanced neon isotope-selective materials.</p> Graphical abstract <p></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

Neon isotope separation in porous \(\gamma\)-\(Al_2\)\(O_3\) at cryogenic temperatures: molecular dynamics insights into pore size and temperature effects

  • Liu Zhonghao,
  • Chen Jiayue,
  • Zhou Beilin

摘要

This study systematically investigates the separation performance of porous \(\gamma\) γ - \(Al_2\) A l 2 \(O_3\) O 3 for neon isotopes ( \(^{20}Ne\) 20 N e / \(^{22}Ne\) 22 N e ) under cryogenic conditions through molecular dynamics (MD) simulations. By constructing \(\gamma\) γ - \(Al_2\) A l 2 \(O_3\) O 3 models with varying pore sizes (4.5–15 Å) and performing MD simulations, the critical effects of pore size and temperature on separation factors are revealed. The results demonstrate that \(\gamma\) γ - \(Al_2\) A l 2 \(O_3\) O 3 with sub-6 Å pore size exhibits remarkable isotopic sieving capability under a fixed pore volume of 0.6 \(\hbox {cm}^3/\hbox {g}\) cm 3 / g . Specifically, the 4.5 Å pore-sized material achieves a separation factor of 1.333 at 30 K, indicating preferential kinetic selectivity for \(^{20}Ne\) 20 N e . Reduced temperatures significantly enhance separation performance, provided that the pore size is sub-10 Å. The diffusion coefficient’s dependence on both temperature and pore diameter follows the Knudsen diffusion mechanism. This research establishes that microporous \(\gamma\) γ - \(Al_2\) A l 2 \(O_3\) O 3 enables effective neon isotope separation through combined molecular sieving and kinetic discrimination effects, offering theoretical foundations for developing advanced neon isotope-selective materials.

Graphical abstract