Use rotating basis vectors with e˙1=Ωe2, e˙2=−Ωe1. The inertial velocity is (x˙1−Ωx2)e1+(x˙2+Ωx1)e2. The two fixed rotating anchors are (0,±a), so the spring lengths are ℓ±=x12+(x2∓a)2. Combining kinetic and elastic energies givesA constant elastic offset has no dynamical effect.
L=2m[(x˙1−Ωx2)2+(x˙2+Ωx1)2]−2k[(ℓ+−l0)2+(ℓ−−l0)2].
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