<p>Unstart dynamics are experimentally investigated in a streamtraced hypersonic inlet at angles of attack, <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\alpha = -5^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <mo>-</mo> <msup> <mn>5</mn> <mo>∘</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\alpha = 0^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <msup> <mn>0</mn> <mo>∘</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\alpha = 3^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <msup> <mn>3</mn> <mo>∘</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. High repetition pressure field imaging and external shock structure imaging are performed to time resolve the unstart shock foot motions and shock train dynamics, which provide mutually evaluating and complementary information about the unstart dynamics. Two distinct unstart responses, referred to as a "weak" and "strong" response, are obtained at low and high back pressure settings. During a weak response, the unstart leading shock was disgorged from the internal passage but oscillated near the cowl closure, with supersonic flow present in the vicinity of the cowl. During a strong response, the unstart shock train is disgorged from the inlet internal passage and the unstart leading shock oscillates in the close vicinity of the inlet leading edge. An entirely subsonic flow entered the inlet internal passage during this response. The influence of angle of attack on the shock dynamics is then evaluated by tracking the unstart leading shock foot. Critical differences were observed in the unstart shock motions and shock velocities between the weak and strong responses for a given angle of attack and for a given response between the different angles of attack. Due to these differences, the unstart duration for a strong response, increased from approximately 11&#xa0;ms to 14&#xa0;ms for <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\alpha = -5^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <mo>-</mo> <msup> <mn>5</mn> <mo>∘</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\alpha = 3^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <msup> <mn>3</mn> <mo>∘</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. The peak unstart shock speed for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\alpha = -5^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <mo>-</mo> <msup> <mn>5</mn> <mo>∘</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> is approximately 20% higher when compared to <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\alpha = 3^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <msup> <mn>3</mn> <mo>∘</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. A new velocity scaling based on the mean inflow velocity at the inlet throat plane makes a better collapse of the peak shock velocity.</p>

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Unstart dynamics of hypersonic Busemann inlet at non-zero angles of attack

  • Matt Schram,
  • Venkat Narayanaswamy

摘要

Unstart dynamics are experimentally investigated in a streamtraced hypersonic inlet at angles of attack, \(\alpha = -5^\circ \) α = - 5 , \(\alpha = 0^\circ \) α = 0 and \(\alpha = 3^\circ \) α = 3 . High repetition pressure field imaging and external shock structure imaging are performed to time resolve the unstart shock foot motions and shock train dynamics, which provide mutually evaluating and complementary information about the unstart dynamics. Two distinct unstart responses, referred to as a "weak" and "strong" response, are obtained at low and high back pressure settings. During a weak response, the unstart leading shock was disgorged from the internal passage but oscillated near the cowl closure, with supersonic flow present in the vicinity of the cowl. During a strong response, the unstart shock train is disgorged from the inlet internal passage and the unstart leading shock oscillates in the close vicinity of the inlet leading edge. An entirely subsonic flow entered the inlet internal passage during this response. The influence of angle of attack on the shock dynamics is then evaluated by tracking the unstart leading shock foot. Critical differences were observed in the unstart shock motions and shock velocities between the weak and strong responses for a given angle of attack and for a given response between the different angles of attack. Due to these differences, the unstart duration for a strong response, increased from approximately 11 ms to 14 ms for \(\alpha = -5^\circ \) α = - 5 to \(\alpha = 3^\circ \) α = 3 . The peak unstart shock speed for \(\alpha = -5^\circ \) α = - 5 is approximately 20% higher when compared to \(\alpha = 3^\circ \) α = 3 . A new velocity scaling based on the mean inflow velocity at the inlet throat plane makes a better collapse of the peak shock velocity.