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In "The Deep" Mr. Pesapane uses stop-motion animation to create a dreamlike, hypnotic facsimile of the ocean depths in which old metal objects — pocket knives, calipers, keys, a mesh purse, a cartridge belt — stand in for slowly moving sea creatures.
In this paper we investigate the behavior of shock-capturing methods for slowly moving shocks.
When the SCR is small, this effect will become more serious for slowly moving targets and the moving targets will be indistinguishable from the clutter.
It is known that for slowly moving shocks even a first-order scheme, such as the Godunov or Roe type methods, will generate downstream oscillatory wave patterns that cannot be effectively damped by the dissipation of these first-order schemes.
Such an effect, originating from the hydrodynamic instability induced by surface tension sensitivity to surface concentration of transferred solute, is mathematically formulated and numerically simulated for slowly moving single spherical drops in an axisymmetric boundary-fitted coordinate system by solving coupled fluid flow and solute mass transfer equations.
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We here address the issue of ground clutter rejection for the detection of slowly moving targets in a non-side looking (NSL) array configuration airborne radar.
In Fig. 5, traces of the user throughput for MIMO 4×4 based on TM4 are shown for different numbers of layers for a slowly moving mobile station (3 km/h) as a function of the distance between the mobile station and the base station.
Detecting a single atom in a high-finesse cavity supporting a mode with a small waist is particularly interesting for a slowly moving atom.
If (P z,a notequiv0) for a slowly moving target function a, that is, (T r, a)=S r, w)), then mbiggl r,frac{1}{w-a}biggr)=S r,w).
These virtues make the algorithm to be an advisable choice for ground slowly moving targets detection in real-world clutter environments.
If (P z,a neq0) for a slowly moving target function a, that is, (T r,a)=S r,w)), then m biggl r,frac{1}{w-a} biggr)=S r,w).
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