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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<br />

α, deg<br />

40 60<br />

C m,α<br />

1.6<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

C m<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

−0.2<br />

0 20 40 60<br />

α, deg<br />

V.B. Spherical Segment Family<br />

0<br />

0 20<br />

α, deg<br />

40 60<br />

C n<br />

0<br />

−0.1<br />

−0.2<br />

−0.3<br />

−0.4<br />

−0.5<br />

−0.6<br />

−0.7<br />

0 20<br />

α, deg<br />

40 60<br />

Figure 7. Sharp Cone Moment Coefficient Validation, β = 20 o .<br />

C n,β<br />

0<br />

−0.5<br />

−1<br />

−1.5<br />

0 20 40 60<br />

α, deg<br />

Figure 8. Sharp Cone Stability Derivative Validation, β = 20 o .<br />

δ c = 5 o<br />

δ c = 15 o<br />

δ c = 30 o<br />

δ c = 5 o (CBA)<br />

δ c = 15 o (CBA)<br />

δ c = 30 o (CBA)<br />

δ c = 5 o<br />

δ c = 15 o<br />

δ c = 30 o<br />

δ c = 5 o (FD)<br />

δ c = 15 o (FD)<br />

δ c = 30 o (FD)<br />

The blunting <strong>of</strong> entry vehicles to reduce aeroheating is <strong>of</strong>ten achieved through the addition <strong>of</strong> a spherical<br />

segment as the nose <strong>of</strong> the vehicle. For common entry vehicles such as sphere-cones and blunted biconics,<br />

the spherical segment family is parametrized by the nose radius, rn, and cone half-angle, δc (Figure 9). The<br />

nose radius and cone half-angle determine the portion <strong>of</strong> the spherical segment used to blunt the vehicle<br />

due to tangency conditions en<strong>for</strong>ced between the spherical segment and conical frustum. The surface <strong>of</strong> the<br />

spherical segment is parametrized by the distance from the origin along the x-axis, u = x, and revolution<br />

angle, v = ω, as shown in Figure 9. The resulting position vector, r, is shown in Eq. (16).<br />

r = [u r 2 n − u 2 cos(v) − r 2 n − u 2 sin(v)] T<br />

10 <strong>of</strong> 19<br />

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

(16)

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