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Aerodynamic Design of Unmanned and Scaled Supersonic ...

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K. Yoshida <strong>and</strong> Y. Makino<br />

minimum pressure drag characteristics were<br />

estimated over the whole Mach number range as<br />

shown in Figure 17. We made best use <strong>of</strong> the nonaxisymmetrical<br />

area-ruled body concept <strong>and</strong><br />

obtained remarkable improvement in aerodynamic<br />

performance. Consequently, the “2.5th<br />

Configuration” was selected as the final<br />

aerodynamic configuration for the NEXST-2<br />

airplane.<br />

2.0th Configuration<br />

2.5th Configuration<br />

3.3 Wind Tunnel Tests<br />

Figure 17. Minimum pressure drag <strong>of</strong> NEXST-2<br />

To underst<strong>and</strong> the strong airframe/nacelle<br />

interference completely, <strong>and</strong> to develop the reliable <strong>and</strong> effective database for supersonic<br />

intake, several wind tunnel tests were conducted [22-24, 26-27]. In this section, principal<br />

results on fundamental research activity except intake tests are summarized below.<br />

1) CFD validation tests <strong>of</strong> the airframe/nacelle<br />

interference configuration model<br />

The test model <strong>of</strong> the “0-8th Configuration” with<br />

flow-through-nacelle was used to conduct the CFD<br />

validation for a complicated configuration with<br />

nacelles. Figure 18 shows the force test model with a<br />

modified intake shape <strong>and</strong> a CFD grid. The scale <strong>of</strong><br />

the test model was 8.3% <strong>of</strong> the NEXST-2 airplane.<br />

Both supersonic <strong>and</strong> subsonic tests were conducted at<br />

JAXA [26]. In the test at flow-through-nacelle<br />

condition, the drag measured by a force balance<br />

should be corrected using the relation <strong>of</strong> momentum<br />

balance <strong>of</strong> internal flow <strong>of</strong> the nacelle.<br />

Figure 19 shows measured <strong>and</strong> corrected drag<br />

polar curves, comparing them with CFD(NS)<br />

computation results. An open circle <strong>and</strong> triangle<br />

symbols indicate test results <strong>of</strong> drag characteristics<br />

without <strong>and</strong> with the internal flow correction<br />

respectively. Our CFD computation results on both<br />

conditions without <strong>and</strong> with the internal flow<br />

correction are fairly smaller than those <strong>of</strong> the test<br />

results. It strongly depends on the turbulence model in<br />

our CFD code. If we assumed the drag characteristics<br />

with an <strong>of</strong>f-set value 0.0049 <strong>of</strong> the minimum drag, we<br />

found very high correlation between those assumed<br />

5.06 million points:<br />

supersonic flow case<br />

Figure 18. W/T model & CFD grid <strong>of</strong><br />

“0-8th configuration”<br />

0.01 0.02 0.03 0.04 0.05 C D<br />

drag polar curves <strong>and</strong> test results. Therefore, the pressure drag characteristics estimated by the<br />

CFD code were well validated.<br />

CL<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

-0.1<br />

NEXST-2-08 : Wing+Body+Nacelle<br />

M=1.7<br />

No Int. Correc.<br />

With Int. Correc.<br />

BWT(20099) NS Off-set(0.0049)<br />

Figure 19. Comparison <strong>of</strong> test <strong>and</strong> CFD<br />

results<br />

17

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