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Analytic Hypersonic Aerodynamics for Conceptual Design of Entry ...

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C l<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

−0.1<br />

−0.2<br />

−0.3<br />

−0.4<br />

−0.5<br />

0 20 40 60<br />

α, deg<br />

C m<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

−0.2<br />

−0.4<br />

−0.6<br />

0 20 40 60<br />

α, deg<br />

C n<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

−0.1<br />

−0.2<br />

−0.3<br />

−0.4<br />

0 20 40 60<br />

α, deg<br />

Figure 17. Sphere-Cone and Blunted Biconic Moment Coefficient Validation, β = 20 o .<br />

VI.C. Example Application Using the Superposition <strong>of</strong> Basic Shapes<br />

Biconic<br />

Sphere−Cone<br />

Biconic (CBA)<br />

Sphere−Cone (CBA)<br />

As shown, basic shapes can be superpositioned to construct full entry bodies commonly used <strong>for</strong> various<br />

entry missions. The analytic relations allow <strong>for</strong> rapid parametric sweeps and shape optimization. As an<br />

example, vehicle designers may be interested in a biconic entry vehicle with a peak L/D <strong>of</strong> 2 subject to<br />

certain geometric constraints.<br />

For this problem, a maximum vehicle height <strong>of</strong> 48 in. and a maximum base diameter <strong>of</strong> 21 in. was<br />

assumed. For a given diameter, an increase in the height would result in a more slender vehicle with higher<br />

peak L/D. There<strong>for</strong>e, in order to maximize the base diameter, the height <strong>of</strong> the vehicle must also be<br />

maximized. Parametric sweeps over a wide range <strong>of</strong> angle <strong>of</strong> attack and zero sideslip were per<strong>for</strong>med <strong>for</strong><br />

various cone half angles, δ1 and δ2, in 1 o increments as well as various base diameters. Contours in peak<br />

L/D <strong>for</strong> the maximum allowable base diameter <strong>of</strong> 21 in. are shown in Figure 18. As shown, no sharp biconic<br />

is capable <strong>of</strong> achieving an L/D <strong>of</strong> 2. A theoretical best L/D <strong>of</strong> only 1.86 could be achieved with δ1 = 18 o<br />

and δ2 = 11 o . Consequently, the base diameter was reduced until a sharp biconic with an L/D <strong>of</strong> 2 was<br />

identified. As shown in Figure 19, an L/D <strong>of</strong> 2 is achieved with d = 19.6, δ1 = 17 o , and δ2 = 10 o . Note<br />

that each point in the contour plots corresponds to a full sweep <strong>of</strong> angles <strong>of</strong> attack, a process that is reduced<br />

from hours using CBAERO to minutes using the analytic relations.<br />

δ 2 , deg<br />

25<br />

20<br />

15<br />

10<br />

5<br />

1.8<br />

1.81.8<br />

1.6<br />

1.4<br />

Peak L/D Contours<br />

Optimal Peak L/D = 1.86<br />

1.8<br />

1.61.6<br />

1.2<br />

1<br />

0.8<br />

1.2<br />

1.41.4<br />

1<br />

0.6<br />

5 10 15 20 25 30 35 40 45<br />

δ , deg<br />

1<br />

Figure 18. Contour <strong>of</strong> Peak L/D <strong>for</strong> d = 21 in.<br />

15 <strong>of</strong> 19<br />

δ 2 , deg<br />

American Institute <strong>of</strong> Aeronautics and Astronautics<br />

25<br />

20<br />

15<br />

10<br />

5<br />

2<br />

1.8<br />

1.6<br />

1.4<br />

Peak L/D Contours<br />

Optimal Peak L/D = 2.01<br />

1.8<br />

1.61.6<br />

1.2<br />

1<br />

1.8<br />

1.2<br />

1.41.4<br />

0.8<br />

1<br />

0.6<br />

5 10 15 20 25 30 35 40 45<br />

δ , deg<br />

1<br />

Figure 19. Contour <strong>of</strong> Peak L/D <strong>for</strong> d = 19.6 in.

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