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Sponsored by: China Academy of Aerospace Aerodynamics
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DING Hao-lin, YI Shi-he, WU Yu-yang, et al. Experimental Investigation on Relationship between Reynolds Number and Aero-Optics Produced by Supersonic Films[J]. PHYSICS OF GASES, 2017, 2(3): 54-63. DOI: 10.19527/j.cnki.2096-1642.2017.03.007
Citation: DING Hao-lin, YI Shi-he, WU Yu-yang, et al. Experimental Investigation on Relationship between Reynolds Number and Aero-Optics Produced by Supersonic Films[J]. PHYSICS OF GASES, 2017, 2(3): 54-63. DOI: 10.19527/j.cnki.2096-1642.2017.03.007

Experimental Investigation on Relationship between Reynolds Number and Aero-Optics Produced by Supersonic Films

  • Nowadays, with development of relevant projects, it is becoming an important proposition how to study high Reynolds effects on the aero-optical distortions. Experiment unit Reynolds number can change from 7.2×106~2.2×108 m-1 by designing a variable Reynolds number aero-optical experiment equipment. A wavefront measurement system based on BOS was assembled, and its temporal resolution can reach to 6 ns. With this system, the measurement results from the plano-convex lens wavefront show that:experimental measurement error compared to the theoretical calculation is within ±4%. The transient wavefronts of supersonic film in nine different Reynolds conditions were measured. The analysis shows that, in high Reynolds condition, Reynolds has obvious effects on the supersonic film aero-optical distortion. OPDrmsRe0.88 was found by function fitting the experimental data, which is similar with the derivation result OPDrmsRe0.9. The distribution features of aero-optical distortion along flow direction were studied by wavelet analysis methods in high Reynolds condition. Low-frequency portion (body signals) of OPDrms decreased firstly then increased, but the volatility of its high frequency portion increased firstly and then decreased. The low-frequency part of OPDrms is primarily affected by the overall structure of the flow field, and the high-frequency part is affected by the spatial distribution of the vortex.
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