<p>High-fidelity microphones can be used to characterize laser-generated microblast waves (“microshocks”) in tabletop experiments. This study probes both spherical and hemispherical microshocks, analogous to height-of-burst or surface-burst geometries, at distances of 1–15&#xa0;cm and laser energies in the range of ~&#xa0; 300–630 mJ under face-on (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1227_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(0^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>0</mn> <mo>∘</mo> </msup> </math></EquationSource> </InlineEquation>) or side-on (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1227_Article_IEq2.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>) microphone orientations. We take a Kingery–Bulmash-style analysis approach and calculate the characteristic fitting parameters for time of arrival of the microshock. Blast waves from these laser energies cover scaled distances of ~&#xa0; 2–50&#xa0;m/<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1227_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {kg}^{\mathrm {1/3}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>kg</mtext> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>3</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>, roughly equivalent to the detonation of a few grams of TNT probed from several meters away. We compare the experimental results to BlastX simulations and tabulated data from a variety of sources. Under this experimental configuration, a 302-mJ laser pulse is equivalent to a TNT charge in the mass range 1–18 <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1227_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\upmu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">μ</mi> </math></EquationSource> </InlineEquation>g and the 628-mJ pulse is within the range 10–45 <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="193_2025_1227_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\upmu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">μ</mi> </math></EquationSource> </InlineEquation>g. This corresponds to a laser energy to shock coupling ratio when compared to 100% TNT equivalence of 1–24% and 7–29%, respectively. This work informs microblast scaling expectations for experiments using laser-induced shock waves as a microscale energetic characterization technique and provides connections between laboratory and free-field detonation testing.</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

Acoustic measurements of laser-induced microshocks: time of arrival to yield estimations

  • E. R. Wainwright,
  • S. W. Dean

摘要

High-fidelity microphones can be used to characterize laser-generated microblast waves (“microshocks”) in tabletop experiments. This study probes both spherical and hemispherical microshocks, analogous to height-of-burst or surface-burst geometries, at distances of 1–15 cm and laser energies in the range of ~  300–630 mJ under face-on ( \(0^{\circ }\) 0 ) or side-on ( \(90^{\circ }\) 90 ) microphone orientations. We take a Kingery–Bulmash-style analysis approach and calculate the characteristic fitting parameters for time of arrival of the microshock. Blast waves from these laser energies cover scaled distances of ~  2–50 m/ \(\hbox {kg}^{\mathrm {1/3}}\) kg 1 / 3 , roughly equivalent to the detonation of a few grams of TNT probed from several meters away. We compare the experimental results to BlastX simulations and tabulated data from a variety of sources. Under this experimental configuration, a 302-mJ laser pulse is equivalent to a TNT charge in the mass range 1–18 \(\upmu \) μ g and the 628-mJ pulse is within the range 10–45 \(\upmu \) μ g. This corresponds to a laser energy to shock coupling ratio when compared to 100% TNT equivalence of 1–24% and 7–29%, respectively. This work informs microblast scaling expectations for experiments using laser-induced shock waves as a microscale energetic characterization technique and provides connections between laboratory and free-field detonation testing.