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Also, for the sake of simplicity, we now assume a maximum spreading length (in time domain, ).
During spreading, solidification occurs at the droplet edge before maximum spreading.
Droplets on surfaces with worse wettabilities recoil more after their maximum spreading radii and even rebound from the surface.
For a maximum spreading length, that is,, based on [11, Equation (18)], the interference term when transmitting real data can be expressed as (26).
Surfaces with better wettabilities have faster spreading and larger maximum spreading radii which result in stronger liquid convection during the dynamic phase.
When all the droplets reach their maximum spreading radii at about 40 μs, the droplet on the 5° contact angle surface has the largest spreading radius of 93 μm and the thinnest liquid film while the maximum spreading radius for the droplet on the 60° contact angle surface is 74 μm.
Similar(40)
Impact dynamics are determined and the maximum spread factor calculated for different Reynolds and Weber numbers.
Once it reaches maximum spread, it becomes so thin that it ruptures, producing fragmented splats.
In particular, we determine the first five maximum spectral radii, the minimum least eigenvalue, and the maximum spread, respectively.
Results show that greater maximum spread diameters are achieved with the higher impact velocities and lower viscosity droplets.
AMOSA is giving the best performance of maximum spread all the times, while ∈-constraint performs the worst.
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