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October 2000 Newsletter - Naval Postgraduate School

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FEATURED PROJECT<br />

JP-10/AEROSOL FOR PULSE DETONATION APPLICATIONS, continued from page 6<br />

successfully detonated a JP-10/air aerosol in a PDE combustor.<br />

Previous research at the laboratory resulted in the first<br />

two-phase detonation of a JP10/oxygen mixture and recent<br />

efforts resulted in the first documented two-phase detonation<br />

of JP-10 and air. The results demonstrate the practicality of<br />

liquid-fuel detonations for PDE applications.<br />

Due to the nature of the combustion process, the mode of<br />

operation for a typical PDE is cyclical. The fuel/<br />

air mixture is loaded into a combustor, rapidly<br />

detonated, and then the products are exhausted.<br />

The resulting pressure behind the detonation wave<br />

presses on the head-end, or thrust wall, of the<br />

combustor to generate thrust. After the combustion<br />

event is complete, the exhaust is expelled<br />

from the combustor and a new fuel/air mixture is<br />

loaded and the procedure repeats. This repeated<br />

fill/detonate/exhaust process typically must occur<br />

at frequencies of 40 Hz or greater to generate a<br />

reasonable thrust level for most systems.<br />

Gaseous systems possess an inherent simplicity<br />

since all of the fuel is already in a vapor state and<br />

is therefore more likely to react rapidly with the<br />

oxidizer, which is required in a detonation wave.<br />

Generally, the energy release must occur within<br />

1cm of the detonation leading shock. If the heat<br />

release occurs too late, the combustion zone<br />

decouples from the shock and the detonation will<br />

likely fail. In a two-phase condition, such as a JP-<br />

10/air aerosol, the fuel must be significantly<br />

vaporized before a substantial reaction can occur.<br />

Calculations indicated that a spray possessing<br />

droplets below 6 microns in diameter would be<br />

required to support a two-phase detonation wave.<br />

The experimental facility used for this work,<br />

shown in Figures 1 and 2, was operated at air flow<br />

rates of up to 1.3 kg/s (3 lbm/s) and provided the<br />

engine with air inlet temperatures of up to 500 K.<br />

The air was heated by a hydrogen vitiator with<br />

make-up oxygen and a maximum outlet temperature<br />

of 725 K. The vitiator outlet was connected<br />

to the engine inlet through a 6.35 cm (2.5 inch)<br />

diameter flex hose. The engine geometry is shown<br />

in Figure 3 with exploded views of selected areas.<br />

The engine inlet choke isolated the vitiator from<br />

pressure oscillations in the main combustor and<br />

allowed for redundant metering of the vitiated air flow. Fuel<br />

was injected just after the inlet choke and was allowed to mix<br />

completely before being discharged into a plenum region and<br />

then injected into the main combustor through a perforated<br />

cone segment in order to provide increased turbulence,<br />

mixing, and partial acoustic isolation.<br />

--continued on page 41<br />

From top to bottom:<br />

Figure 1. Experimental<br />

Layout<br />

Figure 2. Test Cell<br />

View of Experimental<br />

Setup<br />

Figure 3. Pulse<br />

Detonation Engine<br />

Geometry<br />

NPS Research page 7<br />

<strong>October</strong> <strong>2000</strong>

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