research

what is astrodynamics?

three-body problem

Consider a system of three point masses m1m2m3m_1 \geq m_2 \geq m_3 moving in three dimensions, subject to their mutual gravity, e.g., Earth–Moon–spacecraft. This is the three-body problem (3BP). Famously, this system has no general closed-form solution; but there are some simplifications we can apply.

Suppose m3m2m_3 \ll m_2. Then the motion of m1m_1 and m2m_2 (the primaries) are unaffected by the motion of m3m_3. With this, the system can be parameterized with the parameter μ=m2m1+m2\mu = \frac{m_2}{m_1+m_2} and becomes the restricted 3BP (R3BP).

The evolution of two masses under their mutual gravity is well understood to be the conic sections. If the primaries move in circular orbits, then we recover the circular R3BP (CR3BP), where—after some frame changes—the motion of m3m_3 is expressed by the equations x¨=2y˙+x+xU,y¨=2x˙+y+yU,z¨=zU,\begin{aligned} \ddot{x} &= 2\dot{y} + x + \partial_x U, \\ \ddot{y} &= -2\dot{x} + y + \partial_y U, \\ \ddot{z} &= \partial_z U, \end{aligned} where U=(1μ)r13+μr23U = \frac{(1-\mu)}{r_{13}} + \frac{\mu}{r_{23}} is the potential function, ri3r_{i3} is the distance from mass ii to m3m_3, and m1m_1 and m2m_2 are fixed at (μ,0,0)(-\mu, 0, 0) and (1μ,0,0)(1-\mu, 0, 0), respectively.

The rich dynamical structure of the CR3BP manifests as periodic, quasi-periodic, and chaotic motion. My research focuses on understanding this structure.