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ESA Document - Emits - ESA

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Figure 4-70: Dynamic Pressure Over Time (L) and Altitude (R) for Regarded Cases<br />

Figure 4-71: G-Load over Time (L) and Altitude (R) for Regarded Cases<br />

HMM<br />

Assessment Study<br />

Report: CDF-20(A)<br />

February 2004<br />

page 334 of 422<br />

As can be seen in the above figures, the duration of the entry phase varies considerably with the<br />

entry angle. Dynamic pressure and g-load increase sharply for steep entries, and also, the<br />

respective peaks shift towards lower altitudes, as shown in the right-hand plots.<br />

It appears that an entry angle of -4º has a particularly well distributed load characteristics and<br />

therefore low structural load peaks. Of course, this feature will have to be investigated in later<br />

analysis. It might be a mere particularity of the given combination of conditions.<br />

A further entity that needs to be investigated is the thermal load. The peak heat flux can be<br />

expected to rise sharply for a steep entry, analogously to the dynamic pressure and g-load.<br />

Conversely, the total integrated heat load can be expected to be slightly, but not dramatically,<br />

larger for shallow entry angles. Details on that analysis are given in the chapter on<br />

aerothermodynamics in this document.<br />

4.4.1.3.1 Budgets<br />

Table 4-37 shows the characteristics of the aerodynamic entry trajectory for the entry angle<br />

corridor with the assumed aerodynamic reference area of 490.87 m 2 . Parachute deployment takes<br />

place at Mach 2, which is reached at an altitude of 13-15 km above the surface.<br />

The entry velocity is about 10% larger at the shallowest end of the range, where also the longest<br />

phase duration is obtained. Conversely, for the steepest entry, the duration is reduced to 227 s.

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