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Fachgebiet Strömungslehre und Aerodynamik

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Last Update

14 June 2007

 

 

The laws of nature are but the mathematical thoughts of God.
Euclid

 

 

 

Spray impact leads to a creation of a fluctuating liquid layer on a wall. The flow in this layer looks very chaotic. This table is an attempt to classify some possible events which can happen during spray impact onto a cold wall: Cascade of breakups of small drops, drop deposition, corona splash, non-symmetric splash after inclined impact, prompt splash, corona breakup into jets, Faraday jets, drops interactions, capillary waves, film dewetting due to drop impact, film instability leading to the creation of big drops on the substrate, jets appearing during very dense Diesel spray impact.

 

We are going to complete the table as soon as new phenomena will be discovered.

 

 

 

Drop impacting onto a dry rigid substrate creates a radial flow in the lamella. The lamella is bounded by a rim formed due to capillary forces. If the substrate is non-wettable, the rim recedes, sometime leading to rebound.

 

 

Drop impacting onto a liquid film also creates a radial flow in the “inner region” of the film. This flow interacts with the outer undisturbed film. If the inertia is high enough, this interaction leads to the creation of a crown-like uprising sheet. This free sheet is bounded by a rim, formed by capillary forces. At some conditions (above the splashing threshold) the rim centerline bends leading to the formation of cusps, jets and secondary droplets.

 

 

Drop breaks up in a strong, non-stationary gas flow.  Several mechanisms of drop breakup are distinguished:

-       Bag break-up

-       Shear break-up

-       Stretching/thinning break-up

-       Catastrophic break-up

 

 

High velocity gradients and instationary viscous streams can also destroy the drop. The break-up mechanisms are subdivided into

-       Capillary break-up

-       Necking

-       End-pinching

-       Tip streaming

 

 

Binary drop collision leads to the creation of a radially expanding free liquid sheet, bounded by a rim. This rims is formed by surface tension. At some instant the rim recedes, merges and creates a stretching free jet. This jet is bounded by two globes. The globes are also formed by capillary forces.

 

 

 

 

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