bsk-2001 commited on
Commit
2233aa3
·
verified ·
1 Parent(s): 811c56f

Update README.md

Browse files
Files changed (1) hide show
  1. README.md +10 -3
README.md CHANGED
@@ -17,17 +17,24 @@ size_categories:
17
  ## Description
18
 
19
  The dataset captures the time-evolving behavior of 3D spherical droplets subjected to an external shock wave in air.
20
- The interaction with the shock wave results in two different breakup-modes of the droplet (SIE and RTP).
 
 
 
 
 
 
 
21
  Here we investigate a scenario with symmetric boundary conditions at the north, south, top and bottom walls.
22
 
23
  <div style="display:flex;justify-content:center;gap:20px;flex-wrap: wrap;">
24
  <div>
25
  <video style="width:100%;max-width:800px" src="https://huggingface.co/datasets/FluidVerse/3D_SDBA_SSOOSS/resolve/main/SDBA_SSOOSS_RTP_Mas1.20.mp4" loop autoplay muted controls></video>
26
- <p style="position:relative;top:-30px;font-size:14px">Shock-Induced Droplet RTP-Break in Air (Mach 1.20)</p>
27
  </div>
28
  <div>
29
  <video style="width:100%;max-width:800px" src="https://huggingface.co/datasets/FluidVerse/3D_SDBA_SSOOSS/resolve/main/SDBA_SSOOSS_SIE_Mas1.20.mp4" loop autoplay muted controls></video>
30
- <p style="position:relative;top:-30px;font-size:14px">Shock-Induced Droplet SIE-Break in Air (Mach 1.20)</p>
31
  </div>
32
  </div>
33
 
 
17
  ## Description
18
 
19
  The dataset captures the time-evolving behavior of 3D spherical droplets subjected to an external shock wave in air.
20
+ When a shock wave impacts a droplet, the initial response—largely independent of the Weber number—is a deformation phase in which the droplet flattens.
21
+ This interaction with the shock wave results in two different breakup-modes of the droplet (SIE and RTP).
22
+ In the SIE regime, breakup is driven mainly by strong shear forces acting along the droplet surface.
23
+ After the droplet has flattened, shear-induced disturbances emerge near the equator; these instabilities originate near the droplet equator after the droplet has flattened out in the first phase and are advected along the droplet surface.
24
+ As the relative velocity between the droplet and the surrounding gas increases, these disturbances grow due to Kelvin–Helmholtz instability, eventually stripping liquid from the droplet and producing fine droplets downstream.
25
+ In contrast, in the RTP regime, relatively stronger surface tension suppresses the growth of such shear instabilities, maintaining a smoother interface.
26
+ As deformation progresses, the upstream side of the droplet becomes concave as the surrounding gas penetrates and pierces the liquid.
27
+ Unlike RTP, the SIE regime is characterized by a continuous and gradual loss of mass, often resulting in a mist of droplets downstream.
28
  Here we investigate a scenario with symmetric boundary conditions at the north, south, top and bottom walls.
29
 
30
  <div style="display:flex;justify-content:center;gap:20px;flex-wrap: wrap;">
31
  <div>
32
  <video style="width:100%;max-width:800px" src="https://huggingface.co/datasets/FluidVerse/3D_SDBA_SSOOSS/resolve/main/SDBA_SSOOSS_RTP_Mas1.20.mp4" loop autoplay muted controls></video>
33
+ <p style="position:relative;top:-30px;font-size:14px">Shock-Induced Droplet RTP-Breakup in Air (Mach 1.20)</p>
34
  </div>
35
  <div>
36
  <video style="width:100%;max-width:800px" src="https://huggingface.co/datasets/FluidVerse/3D_SDBA_SSOOSS/resolve/main/SDBA_SSOOSS_SIE_Mas1.20.mp4" loop autoplay muted controls></video>
37
+ <p style="position:relative;top:-30px;font-size:14px">Shock-Induced Droplet SIE-Breakup in Air (Mach 1.20)</p>
38
  </div>
39
  </div>
40