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proceedings of the fourth us water jet conference - Waterjet ...

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Our approach to improving <strong>the</strong> performance <strong>of</strong> conventional <strong>water</strong> <strong>jet</strong>s is to<br />

fundamentally modify <strong>the</strong> physical fluid behavior <strong>of</strong> an ordinary, continuo<strong>us</strong> <strong>water</strong> <strong>jet</strong>.<br />

We term <strong>the</strong>se <strong>jet</strong>s "Perc<strong>us</strong>sive Jets."<br />

PERCUSSIVE JETS<br />

General<br />

The photograph in Figure 1 can be <strong>us</strong>ed to ill<strong>us</strong>trate Perc<strong>us</strong>sive Jets in <strong>the</strong>ir<br />

simplest form. The special free-stream characteristics <strong>of</strong> Perc<strong>us</strong>sive Jets shown may be<br />

obtained by modulating <strong>the</strong> discharge <strong>of</strong> <strong>water</strong> through <strong>the</strong> <strong>jet</strong> nozzle, i.e., by cycling <strong>the</strong><br />

discharge flow above and below its average value with some particular frequency,<br />

amplitude, and waveform. Details have been disc<strong>us</strong>sed in References (1), (2), and (3).<br />

Figure 1. Example <strong>of</strong> Perc<strong>us</strong>sive Jets. A small cyclic variation or modulation impressed<br />

on a steady discharge <strong>of</strong> <strong>water</strong> ca<strong>us</strong>es <strong>the</strong> free <strong>jet</strong> to become bunched. Consequently <strong>the</strong><br />

<strong>jet</strong> will strike a target in a sequence <strong>of</strong> sharp impacts ra<strong>the</strong>r than steadily.<br />

In modulated free <strong>jet</strong> discharge, <strong>the</strong> slow and fast portions <strong>of</strong> each discharge cycle<br />

tend to flow toge<strong>the</strong>r or bunch in <strong>the</strong> free stream. The stream th<strong>us</strong> becomes a train <strong>of</strong><br />

bunches <strong>of</strong> <strong>water</strong> which eventually separate. Bunch diameter increases with downstream<br />

distance until <strong>the</strong> axial velocity becomes uniform within each bunch.<br />

At any particular distance from <strong>the</strong> nozzle, <strong>the</strong> free flow produced by modulation<br />

is periodically thicker and thinner than <strong>the</strong> nozzle discharge. Maximum and minimum<br />

diameters depend on downstream distance according to modulation characteristics and to<br />

aerodynamic and surface tension effects. The diameter is a minimum <strong>of</strong> zero for part <strong>of</strong><br />

<strong>the</strong> time if <strong>the</strong> stream bunches have separated.<br />

When this varying free flow strikes a target, <strong>the</strong> momentum flux through <strong>the</strong><br />

nozzle is not transmitted as a steady force, but as a possibly discontinuo<strong>us</strong> sequence <strong>of</strong><br />

force peaks or perc<strong>us</strong>sive impacts. The maximum stream impact area and force at any<br />

distance from <strong>the</strong> nozzle correspond to <strong>the</strong> maximum cross-sectional area produced by<br />

stream bunching up to that distance.<br />

33

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