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Determining Dynamic Stability of a Re-entry Capsule at Free Fall

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Abstract

Re-entry capsules, designed with blunt-body shapes to endure hypersonic air velocities and heat, encounter instability in the low subsonic regime during the final descent phase. Ensuring a controlled descent with the appropriate attitude for deploying deceleration systems becomes paramount. To address this challenge, we employ a cost-effective approach to investigate the dynamic stability of a typical re-entry capsule in free fall. This study involves formulating the aerodynamic model of the system and hypothesizing associated coefficients. A meticulously designed and instrumented prototype is dynamically scaled and subjected to low altitude drop tests to recreate the desired scenario. Subsequently, the data collected during these tests is processed, and stability derivatives are estimated using system identification techniques. Our research contributes to a deeper understanding of the dynamic stability of re-entry capsules during free fall, shedding light on their behavior and providing insights essential for improving their performance and safety during descent.

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Data availability

The data that support the findings of this study are highly confidential in nature, as they are associated with an upcoming space program. Due to security and confidentiality considerations, access to the data is restricted. However, researchers interested in accessing the data may submit requests for access to the corresponding author, subject to approval and in accordance with the policies and guidelines set by Aerotecnica Missili & Spazio.

Abbreviations

\({A}_{ref}\) :

Reference area of the model (m2)

\({C}_{l\dot{\beta }}+{C}_{lp}\) :

Yaw damping coefficient

\({C}_{l}\) :

Yaw coefficient

\({C}_{l\beta }\) :

Yaw coefficient due to sideslip angle

\({C}_{m\dot{\alpha }}+{C}_{mq}\) :

Pitch damping coefficient

\({C}_{m}\) :

Pitch coefficient

\({C}_{m\alpha }\) :

Pitch coefficient due to angle of attack

\({C}_{n}\) :

Roll coefficient

\({C}_{nr}\) :

Roll damping coefficient

\({C}_{n\beta }\) :

Roll coefficient due to sideslip angle

\({C}_{x}\) :

X-axis force coefficient

\({C}_{x\alpha }\) :

X-axis force coefficient due to angle of attack

\({C}_{y}\) :

Y-axis force coefficient

\({C}_{y\beta }\) :

Y-axis force coefficient due to sideslip angle

\({C}_{z}\) :

Z-axis force coefficient

\({C}_{z\alpha }\) :

Z-axis force coefficient due to angle of attack

\({I}_{xx}\) :

X-axis moment of inertia (kg m2)

\({I}_{yy}\) :

Y-axis moment of inertia (kg m2)

\({I}_{zz}\) :

Z-axis moment of inertia (kg m2)

\({g}_{x}\) :

X-axis acceleration due to gravity in the inertial frame (m/s2)

\({g}_{y}\) :

Y-axis acceleration due to gravity in the inertial frame (m/s2)

\({g}_{z}\) :

Z-axis acceleration due to gravity in the inertial frame (m/s2)

\({l}_{CG}\) :

Distance between nose and C.G. (m)

\({m}_{1}\) :

Mass reading from balance 1 (kg)

\({m}_{2}\) :

Mass reading from balance 2 (kg)

\(\dot{p}\) :

X-axis angular acceleration (rad/s2)

\({p}^{*}\) :

X-axis normalized angular rate (rad)

\(\overline{q }\) :

Dynamic pressure (Pa)

\(\dot{q}\) :

Y-axis angular acceleration (rad/s2)

\({q}^{*}\) :

Y-axis normalized angular rate (rad)

\(\dot{r}\) :

Z-axis angular acceleration (rad/s2)

\({r}^{*}\) :

Z-axis normalized angular rate (rad)

\(\dot{u}\) :

Xi-axis acceleration in the inertial frame (m/s2)

\(\dot{v}\) :

Yi-axis acceleration in the inertial frame (m/s2)

\(\dot{w}\) :

Zi-axis acceleration in the inertial frame (m/s2)

\({{\varvec{V}}}_{{\varvec{x}}}\) :

X-axis velocity vector in body frame (m/s)

\({{\varvec{V}}}_{{\varvec{y}}}\) :

Y-axis velocity vector in body frame (m/s)

\({{\varvec{V}}}_{{\varvec{z}}}\) :

Z-axis velocity vector in body frame (m/s)

\(\dot{\alpha }\) :

Angle of attack rate (rad/s)

\({\alpha }_{t}\) :

Total angle (rad)

\(\dot{\beta }\) :

Side-slip angle rate (rad/s)

\(h\) :

Height of the string (m)

\(I\) :

Total moment of inertia (kg m2)

\(M\) :

Mach number

\(T\) :

Time period of one oscillation (s)

\(V\) :

Magnitude of the velocity vector in body frame (m/s)

\(d\) :

Reference diameter of the model (m)

\(g\) :

Acceleration due to gravity (m/s2)

\(l\) :

Length of the model (m)

\(m\) :

Total mass of the model (kg)

\(p\) :

X-axis angular rate (rad/s)

\(q\) :

Y-axis angular rate (rad/s)

\(r\) :

Z-axis angular rate (rad/s)

\(t\) :

Time period (s)

\(\alpha\) :

Angle of attack (rad)

\(\beta\) :

Side-slip angle (rad)

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Acknowledgements

The authors are grateful for the guidance and motivation provided by Mr. K. Srinivasan of the Wind Tunnel Data Division, Wind Tunnel Group, Aeronautics Entity, Vikram Sarabhai Space Centre. This work was supported by Vikram Sarabhai Space Centre, Indian Space Research Organisation.

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Correspondence to C. Priyant Mark.

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Mark, C.P., Netto, W. Determining Dynamic Stability of a Re-entry Capsule at Free Fall. Aerotec. Missili Spaz. 103, 101–116 (2024). https://doi.org/10.1007/s42496-023-00180-7

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