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Moon Landing: Difference between revisions

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Line 17: Line 17:
  \text{subject to} \\
  \text{subject to} \\
\quad \dot{h}(t) & = & v(t),\\
\quad \dot{h}(t) & = & v(t),\\
\quad \dot{v}(t) & = & -1 + \frac{T(t)}{m}, \\
\quad \dot{v}(t) & = & -1 + \frac{T(t)}{m(t)}, \\
\quad \dot{m}(t) & = & -\frac{T(t)}{2.349}, \\
\quad \dot{m}(t) & = & -\frac{T(t)}{2.349}, \\
\quad h(0) &=& 1, \\
\quad h(0) &=& 1, \\

Latest revision as of 17:25, 22 February 2026

Moon Landing
State dimension: 1
Differential states: 3
Discrete control functions: 2


The Moon Landing problem is a simplification of a spacecraft trying to land on the moon's surface. Its objective is to minimize the fuel consumption during the landing maneuver while landing savely on the ground with zero vertical velocity.

The implementation here is taken from [1]. Its dynamics are given by a two-dimensional ODE model.

Mathematical formulation

minT,tfm(tf)subject toh˙(t)=v(t),v˙(t)=1+T(t)m(t),m˙(t)=T(t)2.349,h(0)=1,v(0)=0.783,m(0)=1,tf0,h(tf)=0,v(tf)=0,T(t)[0,1.227] t[0,tf]

Reference Solutions

Here is one local solution to the above control problem.

Miscellaneous and Further Reading

This formulation and a detailed description can be found in [1].

References

[1] Multidisciplinary Optimal Control Library: https://openmdao.org/dymos/docs/latest/examples/moon_landing/moon_landing.html