2208.07790
Dynamics of the no-slip Galton board
J. Ahmed, T. Chumley, S. Cook, C. Cox, H. Grant, N. Petela, B. Rothrock, R. Xhafaj
incompletehigh confidence
- Category
- Not specified
- Journal tier
- Specialist/Solid
- Processed
- Sep 28, 2025, 12:56 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
Both the paper and the model correctly identify the path-reversing 2-periodic criterion γ = (v/ẋ0)(sin θ cos φ − cos θ sin φ) and give coherent proofs (paper via the β-parameter rotation map; model via a −1 eigenvector condition of the no-slip collision matrix). However, both sources misstate the kinematic “range” relation for the required planar speed v: the paper asserts v = 2√(g d) sin 2θ (its Eq. (3)), while the standard constant-acceleration calculation at equal heights gives d = (v^2/g) sin 2θ and hence v = √(g d / sin 2θ). The model reproduces this incorrect closed form as an “equivalent” expression. Thus, the core no-slip criterion is right, but the stated v(g,d,θ) relation needs correction.
Referee report (LaTeX)
\textbf{Recommendation:} minor revisions \textbf{Journal Tier:} specialist/solid \textbf{Justification:} The work provides a clear, verifiable periodicity criterion for forced no-slip wedge billiards and demonstrates how force generates path-reversing 2-cycles. The proof is conceptually clean and consistent with known no-slip mechanics. However, the explicit formula given for the necessary planar speed v (their Eq. (3)) conflicts with the standard equal-height range relation. Correcting this point will reconcile the kinematics and make the theorem fully precise.