The Sun-Earth L2 point is a point beyond the Earth on the
Sun-Earth line where the gravitational forces of the Sun and the
Earth are exactly balanced by centrifugal force. A spacecraft with
a large solar sail is to be placed at an equilibrium point near L2
where the centrifugal force is augmented by the sail force. The
in-plane equations of motion (EOMs), linearized about this
equilibrium point, are
π₯Μ= 2π¦Μ + 12.762π₯
π¦Μ= β2π₯Μ β 4.914π¦ + 1.948π’
where u is the deviation of the solar sail angle from the
nominal (nominal solar sail position is perpendicular to the
Sun-Earth line) at the equilibrium. Here π₯, π¦ are in units of 1.51
Γ 106 km (the distance from the Earth to L2 point), time is in
units of 1/n, where n is Earth angular velocity about the Sun, and
the equilibrium point is 16% closer to Earth than the L2 point.
Problem 1. [30 points] Consider the open-loop system (with π’ =
0). Is the system stable? [Hint: Re-write EOMs in the form πΜ = π΄π
+ π΅π’ where π = [ π₯ π₯Μ π¦ π¦Μ ] π and compute four eigenvalues of the
matrix π΄. Use MATLAB command eig(A). Check their location on the
complex plane]
The Sun-Earth L2 point is a point beyond the Earth on the Sun-Earth line where the gravitational forces of the Sun and t
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The Sun-Earth L2 point is a point beyond the Earth on the Sun-Earth line where the gravitational forces of the Sun and t
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