When , is constant and the system becomesThusFor time dependence , the dispersion relation isExplicitly,and . This is an axisymmetric inertial-acoustic wave: pressure supplies the restoring term and epicyclic motion supplies the term.
Radial buoyancy frequency 2026-10-06
The radial buoyancy frequency describes restoration of a radially displaced parcel in a stratified astrophysical disk. With a dimensionless specific entropy , its square is proportional to . Negative means an adverse entropy stratification, but epicyclic motion can still stabilize the parcel. For smooth thin disk profiles, is usually of order .
If the prescribed gas velocity is itself a free epicyclic motion solution, subtract its two momentum equations from the forced dust epicycle with aerodynamic drag equations. The velocity difference obeys a damped epicycle and decays as . Therefore dust approaches the gas velocity with identical phase and amplitude for every positive drag rate. At zero drag the difference does not decay, so the late-time limit is nonuniform as drag vanishes. A finite-wavelength inertial-acoustic wave is detuned from the free epicycle; matching its phase and amplitude in the weak-drag limit additionally requires . For a gas density wave of frequency , the exact radial transfer amplitude isobtained by solving the two dust equations and using . At it is exactly one.
Velocity-kick epicycle Created 2026-10-06 Updated 2026-10-14
A small planar velocity kick on a stellar circular orbit produces a local epicyclic motion in the source's rotating reference frame. With outward , forward , and initial displacements zero, Hill equations give and . Tangential kicks combine an epicycle with Keplerian shear; a radial kick gives a closed leading-order epicyclic ellipse.