• High Power Laser Science and Engineering
  • Vol. 9, Issue 2, 02000e14 (2021)
Ai Du1、2、*, Yi Ma1、2, Mingfang Liu1、2, Zhihua Zhang1、2, Guangwei Cao3, Hongwei Li3, Ling Wang4、5, Peijian Si4, Jun Shen1、2, and Bin Zhou1、2
Author Affiliations
  • 1Shanghai Key Laboratory of Special Artificial Microstructure Materials and Technology, Tongji University, Shanghai200092, China
  • 2School of Physics Science and Engineering, Tongji University, Shanghai200092, China
  • 3National Space Science Center, Chinese Academy of Sciences, Beijing100190, China
  • 4Hangzhou Dianzi University, Hangzhou310018, China
  • 5Hangzhou Regenovo Biotechnology Co., Ltd., Hangzhou310038, China
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    DOI: 10.1017/hpl.2020.54 Cite this Article Set citation alerts
    Ai Du, Yi Ma, Mingfang Liu, Zhihua Zhang, Guangwei Cao, Hongwei Li, Ling Wang, Peijian Si, Jun Shen, Bin Zhou. Morphology analysis of tracks in the aerogels impacted by hypervelocity irregular particles[J]. High Power Laser Science and Engineering, 2021, 9(2): 02000e14 Copy Citation Text show less
    SEM images of irregularly shaped Al2O3 grains of (a) Particles-100 and (c), (d) Particles-200 (with surface holes) used as projectiles in the PG experiment. (b) Al2O3 grains on Mylar film.
    Fig. 1. SEM images of irregularly shaped Al2O3 grains of (a) Particles-100 and (c), (d) Particles-200 (with surface holes) used as projectiles in the PG experiment. (b) Al2O3 grains on Mylar film.
    Schematic diagram of projectile flight in the PG.
    Fig. 2. Schematic diagram of projectile flight in the PG.
    Contrast figures for the landing surface of the targets (a) before and (b) after impact.
    Fig. 3. Contrast figures for the landing surface of the targets (a) before and (b) after impact.
    Observation of the track entrance: (a) attachments of Mylar near the track entrance marked by red circles: (b) near circular entrance hole of a penetration track; (c), (e), (f) irregular shape of penetration entrance hole; (d) unclear observation of entrance by VMM; (f) three-dimensional graph matching with (e).
    Fig. 4. Observation of the track entrance: (a) attachments of Mylar near the track entrance marked by red circles: (b) near circular entrance hole of a penetration track; (c), (e), (f) irregular shape of penetration entrance hole; (d) unclear observation of entrance by VMM; (f) three-dimensional graph matching with (e).
    (a), (b) Morphology of entrance holes by impactors and (c), (d) part of track along the impact direction by SEM. The red arrow is marked at the point of observation.
    Fig. 5. (a), (b) Morphology of entrance holes by impactors and (c), (d) part of track along the impact direction by SEM. The red arrow is marked at the point of observation.
    Summary of results: (a) plots of the diameter of original and captured projectiles; (b) plots of measured track lengths shown as a function of aerogel target density, all at 2.3 and 7 km/s by impacting (measurement error is 0.002 mm); (c) the aerogel track lengths () normalized to projectile diameter () against target bulk density; (d) penetration track length scaled () against density ratio ().
    Fig. 6. Summary of results: (a) plots of the diameter of original and captured projectiles; (b) plots of measured track lengths shown as a function of aerogel target density, all at 2.3 and 7 km/s by impacting (measurement error is 0.002 mm); (c) the aerogel track lengths () normalized to projectile diameter () against target bulk density; (d) penetration track length scaled () against density ratio ().
    Aerogel tracks created by impacts of Al2O3 obtained by VMM, the impact direction is from the right (except in (e)): (a) the near-spherical captured projectile with the relatively straight track; (b) a near-spherical particle on the terminal track; (c), (d) the irregular captured projectile with the relatively straight track; (e) the detail of track by impact at 2.3 km/s on 182 mg/cm3; (f) flat-shaped projectile residue on the curved track; (g), (h) the residual grain slightly reduced on the curved track; (i) fine features of a track in the aerogel.
    Fig. 7. Aerogel tracks created by impacts of Al2O3 obtained by VMM, the impact direction is from the right (except in (e)): (a) the near-spherical captured projectile with the relatively straight track; (b) a near-spherical particle on the terminal track; (c), (d) the irregular captured projectile with the relatively straight track; (e) the detail of track by impact at 2.3 km/s on 182 mg/cm3; (f) flat-shaped projectile residue on the curved track; (g), (h) the residual grain slightly reduced on the curved track; (i) fine features of a track in the aerogel.
    The simplified diagram classified from impact tracks (the impact direction is from the left).
    Fig. 8. The simplified diagram classified from impact tracks (the impact direction is from the left).
    The projectile-breakage situation outside of available data of track classification (the impact direction is from the right): (a) two adjacent grains injected simultaneously into the target, the track branch is not caused by particle breakage; (b) three branches at the track tail caused by a projectile rupture; (c) larger particles and smaller ruptured grains remaining in the track tail; (d) tiny grains spread forward in the local enlargement of (c); (e) simplified diagram of the track shown in (b).
    Fig. 9. The projectile-breakage situation outside of available data of track classification (the impact direction is from the right): (a) two adjacent grains injected simultaneously into the target, the track branch is not caused by particle breakage; (b) three branches at the track tail caused by a projectile rupture; (c) larger particles and smaller ruptured grains remaining in the track tail; (d) tiny grains spread forward in the local enlargement of (c); (e) simplified diagram of the track shown in (b).
    Aerogel tracks created by impacts of Al2O3 at 7 km/s (the impact direction is from the right). (a) A track-scan photograph along the impact direction. (b) The track photograph just passing through the two spherical bubbles near the cylindrical aerogel side obtained by VMM. (c), (d) The two segments of the track of (b) revealed by OCT.
    Fig. 10. Aerogel tracks created by impacts of Al2O3 at 7 km/s (the impact direction is from the right). (a) A track-scan photograph along the impact direction. (b) The track photograph just passing through the two spherical bubbles near the cylindrical aerogel side obtained by VMM. (c), (d) The two segments of the track of (b) revealed by OCT.
    ShootAerogelProjectileVelocity
    numberdensity (kg/m3)size(km/s)
    #1117Particles-100~7
    #A112Particles-200~2.3
    #2137Particles-100~7
    #B140Particles-200~2.3
    #3180Particles-100~7
    #C182Particles-200~2.3
    #D100Particles-200~2.3
    Table 1. List of experimental conditions.
    Ai Du, Yi Ma, Mingfang Liu, Zhihua Zhang, Guangwei Cao, Hongwei Li, Ling Wang, Peijian Si, Jun Shen, Bin Zhou. Morphology analysis of tracks in the aerogels impacted by hypervelocity irregular particles[J]. High Power Laser Science and Engineering, 2021, 9(2): 02000e14
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