NO PLIF Visualizations of the Orion Capsule in LENS-I

Combs, Christopher S.; Clemens, Noel T.; Danehy, Paul M.; Bathel, Brett F.; Parker, Ronald A.; Wadhams, Tim P.; Holden, Michael; Kirk, Benjamin S.

doi:10.2514/6.2013-33

Cited by 7 publications

(1 citation statement)

References 23 publications

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“…16 PLIF has also been used to investigate various capsule geometries in high speed flows. [17][18][19][20] Naphthalene PLIF was originally introduced as a fuel-marking technique in low-speed reacting flow experiments 21 but only recently has the technique been used to image ablation products in a supersonic turbulent boundary layer. 3 NASA researchers have used NO PLIF to simulate the ablation process by transpiring NO gas through a port on the surface of a capsule model.…”

Section: Introductionmentioning

confidence: 99%

Development of Naphthalene PLIF for Visualizing Ablation Products from a Space Capsule Heat Shield

Combs

Clemens²,

Danehy

2014

52nd Aerospace Sciences Meeting

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The Orion Multi-Purpose Crew Vehicle (MPCV) will use an ablative heat shield. To better design this heat shield and others that will undergo planetary entry, an improved understanding of the ablation process would be beneficial. Here, a technique developed at The University of Texas at Austin that uses planar laser-induced fluorescence (PLIF) of a low-temperature sublimating ablator (naphthalene) to enable visualization of the ablation products in a hypersonic flow is applied. Although high-temperature ablation is difficult and expensive to recreate in a laboratory environment, low-temperature sublimation creates a limited physics problem that can be used to explore ablation-product transport in a hypersonic flow-field. In the current work, a subscale capsule reentry vehicle model with a solid naphthalene heat shield has been tested in a Mach 5 wind tunnel. The PLIF technique provides images of the spatial distribution of sublimated naphthalene in the heat-shield boundary layer, separated shear layer, and backshell recirculation region. Visualizations of the capsule shear layer using both naphthalene PLIF and Schlieren imaging compared favorably. PLIF images have shown high concentrations of naphthalene in the capsule separated flow region, intermittent turbulent structures on the heat shield surface, and interesting details of the capsule shear layer structure. It was shown that, in general, the capsule shear layer appears to be more unsteady at lower angels of attack. The PLIF images demonstrated that during a wind tunnel run, as the model heated up, the rate of naphthalene ablation increased, since the PLIF signal increased steadily over the course of a run. Additionally, the shear layer became increasingly unsteady over the course of a wind tunnel run, likely because of increased surface roughness but also possibly because of the increased blowing. Regions with a relatively low concentration of naphthalene were also identified in the capsule backshell recirculation region and are most likely the result of cross-flow-induced vortices on the capsule afterbody.

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