Acoustic Wake in a Stratified Ocean: Why Satellites Die Faster Than We Thought ✛ ✎

Original: "Dynamical friction in stratified stellar envelopes"
· Damien Gagnier
arXiv:2607.16422v1 · 2026-07-17 · arXiv non-exclusive · independent analysis · 3 min
Accounting for the stratified structure of giant star envelopes shows that gravitational dynamical friction depends on the global acoustic pattern, not just local density, and the infall time of a satellite can shrink by factors.

A tiny satellite, like a swimmer, cuts through invisible layers of gas in the bloated envelope of a red giant. Each orbit excites an acoustic wake — compression waves traveling through plasma. According to Law of Universal Gravitation, the satellite attracts the gas, and the gas attracts the satellite, creating this wake. This is how gravity works — a key mechanism in the evolution of close binary star systems and the fate of exoplanet planets falling into stellar interiors. As early as Fritz Zwicky realized that dynamical friction governs the motion of galaxies in clusters, and Subrahmanyan Chandrasekhar derived its formula for stars. However, classical recipes assumed a homogeneous medium and rectilinear motion. For a satellite orbiting in a stellar evolution giant's envelope, this is too crude.

The gas density at half the radius of a red giant is about 10⁻⁷ g/cm³, similar to air at an altitude of 150 kilometers. But even in such a rarefied medium, an acoustic wake forms surprisingly efficiently.

The author constructs a linear barotropic acoustic model. The orbit obeys Kepler's third law. The enthalpy perturbation is expanded in spherical harmonics and Fourier modes, and the force is written as a sum over multipoles. The key tool is a retarded Green's function. The calculation is performed for single and binary satellites on circular orbits in power-law density profiles and realistic models of stellar evolution. It turns out that stellar evolution changes dynamical friction not only through local density and Mach number but also through the global structure of the acoustic wake. The radial component of the force is determined by large-scale wave asymmetry and can differ from the homogeneous case even in sign. The azimuthal component, responsible for braking, retains sensitivity to small scales — the so-called Coulomb logarithm. In binary systems, a companion satellite can noticeably alter the radial force and weaken the braking. A local Coulomb-type contribution is absent, so the effect appears only on large scales.

The sound speed in the giant's envelope is about 10 km/s. The orbital speed of the satellite can reach Mach 12, meaning it moves twelve times faster than sound waves, leaving a conical wake similar to that of a supersonic aircraft.

For astrophysicists, this means that the inspiral time of a satellite into a giant's envelope cannot be estimated by knowing only conditions at the orbital point. The wave pattern throughout the entire envelope must be taken into account. The computed infall time for red giant and supergiant models turned out to be shorter than standard homogeneous formulas give. Planetary migration in stellar envelopes proceeds faster than previously thought. The next step is to couple the acoustic response with orbital evolution, allowing the satellite to migrate and change eccentricity. Furthermore, it is necessary to go beyond the linear approximation: where waves become shocks, three-dimensional numerical simulation hydrodynamic simulations will be required. Then it will become clear how law of conservation of angular momentum exchange between waves and orbit shapes the fate of the system. And then the acoustic wake in the stratified ocean will no longer be a mystery.

In the uniform-medium limit, the azimuthal force diverges as resolution increases — the famous Coulomb logarithm from plasma physics. For circular orbits, the maximum scale of the wake is set by the orbital radius, not infinite as in straight-line motion. So the logarithm gets cut off differently.

The theme of planets inside stars evokes Stanisław Lem's novel *Solaris*: a sentient ocean that reacts to human presence. Here, the ocean is plasma, and the 'intellect' is a mathematical calculation that lets us peer into invisible processes.

\mathcal{M} = \frac{\Omega a}{c_s(a)}
Ratio of orbital speed to local sound speed
I_\mathcal{M} = -\frac{\sqrt{2}c_s^2 F_+}{4\pi G^2 M^2 \rho_0}
Dimensionless measure of the azimuthal and radial components
\dot{a} = \frac{a F_\phi}{dL/da}
Rate of change of orbital radius under tangential braking
Scientists
David CharbonneauIsaac NewtonJohannes KeplerWilliam BoruckiSubrahmanyan ChandrasekharRainer Sachs
Concepts
dynamical friction stellar wobble envelope protoplanetary disk dynamics