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Infrared signature studies of aerospace vehicles - DSpace at IIT ...

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adi<strong>at</strong>ion from an engine exhaust plume, based on<br />

the combin<strong>at</strong>ion <strong>of</strong> radi<strong>at</strong>ion from the surface and<br />

the gaseous plume. The modelling determines the<br />

complic<strong>at</strong>ed geometry <strong>of</strong> the radi<strong>at</strong>ing volume<br />

consisting <strong>of</strong> jet and nozzle surfaces. The model<br />

predicts important peaks (which are experimentally<br />

valid<strong>at</strong>ed) <strong>at</strong> 2.7 and 4.3 mm, corresponding to<br />

emission from CO2. A peak <strong>at</strong> 5.8 mm is also<br />

predicted th<strong>at</strong> corresponds to nozzle surface radi<strong>at</strong>ion<br />

<strong>at</strong> its temper<strong>at</strong>ure [61]. The Standardized<br />

<strong>Infrared</strong> Radi<strong>at</strong>ion Model (SIRRM) code developed<br />

under JANNAF (Joint Army Navy NASA<br />

Air Force) project, predicts IR radi<strong>at</strong>ion from<br />

missile and aircraft plumes [72]. The code also<br />

predicts the effect <strong>of</strong> carbon particles on IR<br />

emission characteristics <strong>of</strong> plume. Bakker et al.<br />

[73] gave a brief methodology for computing plume<br />

IR <strong>sign<strong>at</strong>ure</strong>s from naval ship gas turbine engines,<br />

using NATO’s NPLUME program for exhaust field<br />

comput<strong>at</strong>ions.<br />

Hypothetical band models for plume IR-radi<strong>at</strong>ion<br />

modelling are classified into narrow-band and<br />

wide-band models. Wide-band models are used for<br />

obtaining total quantities, while narrow-band models<br />

are used for spectral inform<strong>at</strong>ion [61]. Ibgui and<br />

Hartmann [74] and Ibgui et al. [75] developed an<br />

optimized line-by-line FORTRAN code for the<br />

calcul<strong>at</strong>ion <strong>of</strong> aircraft plume IR <strong>sign<strong>at</strong>ure</strong>. The<br />

results obtained by the model were in good agreement<br />

with the measured labor<strong>at</strong>ory simul<strong>at</strong>ion<br />

results. Soufiani and Taine [76] obtained the emis-<br />

.sivity <strong>of</strong> gases resulting from hydrocarbon combustion<br />

by using a st<strong>at</strong>istical narrow-band model,<br />

which provides fast results <strong>at</strong> reasonable accuracy<br />

[77]. The effect <strong>of</strong> Line Doppler Shift (LDS) is<br />

important when there is a rel<strong>at</strong>ive velocity between<br />

radi<strong>at</strong>ing gas layers, e.g. aircraft plume [77].<br />

Consider<strong>at</strong>ion <strong>of</strong> LDS-effect on plume IR predictions<br />

using narrow-band model shows apparent<br />

increase in radiance compared to calcul<strong>at</strong>ions by<br />

line-by-line techniques [77].<br />

Comput<strong>at</strong>ional Fluid Dynamics (CFD) simul<strong>at</strong>ion<br />

<strong>of</strong> aircraft plumes for obtaining temper<strong>at</strong>ure,<br />

pressure, and concentr<strong>at</strong>ion distributions is also<br />

reported [78]. It is inferred th<strong>at</strong> the spectral intensity<br />

<strong>of</strong> aircraft plumes as received by IR-guided SAMs<br />

in non-afterburning mode, is prominent only in the<br />

4.14–4.45 mm band (Fig. 12) [79]. In non-afterburning<br />

mode, the IRSL from the plume is much<br />

lower than from the tail-pipe and rear fuselage,<br />

which is contrary to popular belief. Further, there is<br />

no emission from gaseous plumes in the 8–12 mm<br />

ARTICLE IN PRESS<br />

Radiance Intensity (W m -2 ⋅Sr -1 ⋅μm -1 )<br />

160<br />

120<br />

80<br />

40<br />

0<br />

0 4 8 12 16 20<br />

λ (μm)<br />

Fig. 12. Spectral radiance intensity <strong>of</strong> aircraft plume (after [79]).<br />

band (even in afterburning mode); but solid surfaces<br />

being grey, emit <strong>at</strong> all wavelengths <strong>at</strong> all temper<strong>at</strong>ures.<br />

Plume IR <strong>sign<strong>at</strong>ure</strong>s were measured experimentally<br />

by Cogliandro and Castelli [80], using<br />

Rolls-Royce GEM.2-MK.1000 engine delivering<br />

750 hp. Comparison <strong>of</strong> experimental results with<br />

theoretical results showed th<strong>at</strong> the experimental<br />

results in 1–14.5 mm band are accur<strong>at</strong>e within 10%.<br />

The IR emission from rocket plumes is <strong>of</strong> interest<br />

for its role in base he<strong>at</strong>ing and engine performance<br />

diagnostics. It is also <strong>of</strong> importance in str<strong>at</strong>egic<br />

functions like early warning, surveillance, acquisition,<br />

and tracking [81,82]. Parameters affecting<br />

plume IR <strong>sign<strong>at</strong>ure</strong> can be grouped into four<br />

c<strong>at</strong>egories, viz. engine, vehicle, flight, and ambient.<br />

The engine parameters are mass flow r<strong>at</strong>e, propellant<br />

type, mixture r<strong>at</strong>io (r<strong>at</strong>io <strong>of</strong> oxidizer mass to<br />

fuel mass), chamber pressure, area r<strong>at</strong>io, and nozzle<br />

contour. Vehicle parameters include number <strong>of</strong><br />

nozzles, nozzle spacing, cant angle, and base<br />

diameter. Altitude, velocity, and angle <strong>of</strong> <strong>at</strong>tack<br />

are flight parameters; and solar azimuth/elev<strong>at</strong>ion<br />

and earthshine/sunshine/skyshine are ambient parameters<br />

[81]. A rocket plume radi<strong>at</strong>es strongly near<br />

4.3 mm, because <strong>of</strong> the CO2 band; but burning <strong>of</strong><br />

combustible species is most striking in missiles flying<br />

below 30 km [83]. Due to this continuing combustion<br />

reaction after the nozzle exit, the plume<br />

temper<strong>at</strong>ure and IR <strong>sign<strong>at</strong>ure</strong> are raised [84–86].<br />

The IR emission from rocket plume is sensitive to<br />

concentr<strong>at</strong>ion <strong>of</strong> carbon particles in the plume. For<br />

the same concentr<strong>at</strong>ion <strong>of</strong> carbon particles, vari<strong>at</strong>ion<br />

in their size has no effect on IR emissions from<br />

the plume [84]. High altitude plume radi<strong>at</strong>es more<br />

IR <strong>sign<strong>at</strong>ure</strong> than <strong>at</strong> sea level; because for same<br />

nozzle exit conditions, high altitude plumes are<br />

bigger than the plume <strong>at</strong> sea level [87].<br />

231

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