Derives constraints on Le Sage screening gravity, showing its predictions in planetary bodies, indicating its falsification.
We derive quantitative constraints on Le Sage-type screening gravity, in which an isotropic background field with mass-proportional attenuation produces gravitational attraction. A minimal model with five assumptions (isotropy, linear Beer–Lambert screening, no self-screening, no re-emission, and instantaneous propagation) exactly reproduces Newton’s inverse-square law for spherical mass distributions, including a direct proof of the shell theorem from the screening integral. For oblate spheroids, nonlinear corrections of the form δF/F = R(ε) τchar arise, where ε is the oblateness and τchar = σρ a is the characteristic optical depth. The isotropic part of this correction is absorbed into the measured gravitational constant and is unobservable; the geometry-dependent residual C(ε) = R(ε) − R(0) constitutes the observable non-Newtonian signal. Because optical depth τchar = σρ a differs between solar system bodies, the model predicts body-dependent effective gravitational parameters (GM)eff . Comparing Earth and Jupiter, the predicted fractional difference |ΔG/G| = 3.76 °ø 10−2 at screening cross section σ = 10−12 m2/kg exceeds the precision of Juno’s determination of Jupiter’s GM by a factor of 3.8 °ø 106. The model is falsified for all cross sections above σcrit = (2.8°æ0.2)°ø10−19 m2/kg; below this threshold, it is indistinguishable from Newtonian gravity at current precision.
No takes yet. Share an insight, caveat, or question.
John Payton Beans (2026) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: