<p>This work presents the experimental investigation of the influence of methane addition to <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\({\hbox {CH}}_{{4}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>CH</mtext> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation>–<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {H}_{{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>H</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>–air mixture (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi = 0.8\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>φ</mi> <mo>=</mo> <mn>0.8</mn> </mrow> </math></EquationSource> </InlineEquation>–1.6) on the critical conditions for transition to detonation in a <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(90^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>90</mn> <mo>∘</mo> </msup> </math></EquationSource> </InlineEquation> wedge. Similar to <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {H}_{{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>H</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>–air mixtures investigated previously, for <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\({\hbox {CH}}_{{4}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>CH</mtext> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation>–<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\hbox {H}}_{{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>H</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>–air mixtures results showed three ignition modes: (i) flame ignition with ignition delay time longer than 1&#xa0;µs, (ii) strong ignition with instantaneous transition to detonation, and (iii) weak ignition with delayed transition to detonation. In a stoichiometric mixture with 5% <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\({\hbox {CH}}_{{4}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>CH</mtext> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation> (i.e., 95% <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\hbox {H}}_{{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>H</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> in fuel), the transition to detonation corresponds to a shock velocity of roughly 752&#xa0;m/s (an increase of 37&#xa0;m/s from that obtained in <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {H}_{{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>H</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>–air) corresponding to <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq13.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="70" /> </InlineMediaObject> <EquationSource Format="TEX">\(M = 1.89\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.89</mn> </mrow> </math></EquationSource> </InlineEquation>. In general, 5% <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq14.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {CH}_{{4}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>CH</mtext> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation> addition caused an increase of 3.25–5.03% in the critical shock wave velocity necessary for transition to detonation for all lean and rich mixtures considered. Also, similar to that found for <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1217_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\hbox {H}}_{{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>H</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>–air mixtures, the transition-to-detonation velocity increased for a leaner and richer mixture. Moreover, it was observed that methane addition in general increased the pressure limit at the wedge tip necessary for the transition to detonation.</p>

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Effect of methane addition to hydrogen–air mixtures on the transition to detonation due to shock wave focusing in a \(90^{\circ }\) wedge

  • S. Khair Allah,
  • W. Rudy,
  • A. Teodorczyk

摘要

This work presents the experimental investigation of the influence of methane addition to \({\hbox {CH}}_{{4}}\) CH 4 \(\hbox {H}_{{2}}\) H 2 –air mixture ( \(\varphi = 0.8\) φ = 0.8 –1.6) on the critical conditions for transition to detonation in a \(90^{\circ }\) 90 wedge. Similar to \(\hbox {H}_{{2}}\) H 2 –air mixtures investigated previously, for \({\hbox {CH}}_{{4}}\) CH 4 \({\hbox {H}}_{{2}}\) H 2 –air mixtures results showed three ignition modes: (i) flame ignition with ignition delay time longer than 1 µs, (ii) strong ignition with instantaneous transition to detonation, and (iii) weak ignition with delayed transition to detonation. In a stoichiometric mixture with 5% \({\hbox {CH}}_{{4}}\) CH 4 (i.e., 95% \({\hbox {H}}_{{2}}\) H 2 in fuel), the transition to detonation corresponds to a shock velocity of roughly 752 m/s (an increase of 37 m/s from that obtained in \(\hbox {H}_{{2}}\) H 2 –air) corresponding to \(M = 1.89\) M = 1.89 . In general, 5% \(\hbox {CH}_{{4}}\) CH 4 addition caused an increase of 3.25–5.03% in the critical shock wave velocity necessary for transition to detonation for all lean and rich mixtures considered. Also, similar to that found for \({\hbox {H}}_{{2}}\) H 2 –air mixtures, the transition-to-detonation velocity increased for a leaner and richer mixture. Moreover, it was observed that methane addition in general increased the pressure limit at the wedge tip necessary for the transition to detonation.