Characterization of Rocking Block Behaviors with Classical and Alternative Restitution Models
Pith reviewed 2026-06-27 05:05 UTC · model grok-4.3
The pith
The choice of restitution model strongly influences the predicted dynamics of rocking blocks under harmonic excitation.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Formulating the rocking block as a hybrid non-smooth dynamical model and analyzing it via bifurcation diagrams, Lyapunov exponents, and basins of attraction shows that the alternative restitution formulation leads to an earlier onset and greater prevalence of complex oscillations as well as changes in the type, stability, and accessibility of attractors compared with the classical Housner model; the dynamical features produced by both formulations converge as the slenderness ratio increases.
What carries the argument
Comparison of the classical Housner restitution coefficient with the Mao et al. alternative formulation inside a hybrid non-smooth dynamical model of the rocking block.
Load-bearing premise
That the hybrid non-smooth formulation and the chosen numerical diagnostics fully capture and correctly classify all relevant behaviors across the parameter ranges examined.
What would settle it
Running controlled rocking-block experiments with measured impact restitution values and checking whether the observed onset of complex oscillations matches the alternative model's predictions more closely than the classical model's predictions.
read the original abstract
This work investigates how restitution modeling affects the dynamics of rocking blocks subjected to harmonic excitation. While several studies have reported discrepancies between experimentally observed impact behavior and the predictions obtained using the classical Housner restitution coefficient, the implications of adopting alternative restitution formulations on the global dynamics of rocking systems remain largely unexplored. The system is formulated as a hybrid non-smooth dynamical model and analyzed through bifurcation diagrams, Lyapunov exponents, and basins of attraction for different slenderness ratios. By comparing the classical restitution model proposed by Housner with the alternative formulation of Mao et al., we show that the choice of restitution model strongly influences the predicted system response. The alternative formulation leads to an earlier onset and greater prevalence of complex oscillations, as well as changes in the type, stability, and accessibility of attractors compared to the classical model. However, as the slenderness ratio increases, the dynamical features produced by both formulations progressively converge, indicating a reduced sensitivity to the restitution model for taller blocks. These results provide a dynamical perspective on why alternative restitution formulations, which predict impact responses closer to experimental observations, can produce markedly different behaviors from those obtained using the classical Housner model.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper formulates rocking blocks under harmonic excitation as hybrid non-smooth systems and compares the classical Housner restitution coefficient against the Mao et al. alternative via bifurcation diagrams, Lyapunov exponents, and basins of attraction across slenderness ratios. It claims the alternative model produces earlier onset and greater prevalence of complex oscillations together with changes in attractor type, stability, and accessibility, while both models converge for larger slenderness ratios.
Significance. If the numerical diagnostics are shown to be accurate, the work supplies a concrete dynamical-systems explanation for why restitution models that better match experiments can yield qualitatively different global responses, with direct relevance to the modeling of rocking structures in seismic engineering.
major comments (2)
- [Lyapunov exponent calculation] The section describing the computation of Lyapunov exponents does not mention insertion of the saltation matrix at each impact event. In hybrid non-smooth systems the standard variational equations must be corrected by the saltation matrix to obtain the correct linearization across velocity discontinuities; omission of this step renders the reported exponents (and therefore the claimed differences in stability and the onset of complex oscillations) unreliable, especially near grazing or chattering regimes highlighted in the abstract.
- [Numerical diagnostics and results] The basins-of-attraction and bifurcation-diagram results are presented without reported checks on integration tolerance, event-detection accuracy, or comparison against an independent event-driven integrator. Because the central claim rests on quantitative differences between the two restitution maps, the absence of such verification leaves open the possibility that the reported attractor changes are sensitive to numerical implementation details.
minor comments (2)
- [Abstract] The abstract is information-dense; a short sentence stating the specific ranges of slenderness ratio and excitation amplitude examined would improve readability.
- [Model formulation] Notation for the two restitution coefficients should be introduced once with a clear equation reference rather than repeated in prose.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments. We address each major point below and will revise the manuscript to improve the description and verification of our numerical methods.
read point-by-point responses
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Referee: [Lyapunov exponent calculation] The section describing the computation of Lyapunov exponents does not mention insertion of the saltation matrix at each impact event. In hybrid non-smooth systems the standard variational equations must be corrected by the saltation matrix to obtain the correct linearization across velocity discontinuities; omission of this step renders the reported exponents (and therefore the claimed differences in stability and the onset of complex oscillations) unreliable, especially near grazing or chattering regimes highlighted in the abstract.
Authors: We acknowledge the omission in the manuscript description. Our implementation follows the standard hybrid-system procedure and inserts the saltation matrix at each impact to linearize across velocity jumps. We will revise the Lyapunov-exponent section to include an explicit description of the saltation matrix, its formula, and its application within the variational equations. This addition will confirm that the reported exponents correctly account for discontinuities, particularly near grazing and chattering. revision: yes
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Referee: [Numerical diagnostics and results] The basins-of-attraction and bifurcation-diagram results are presented without reported checks on integration tolerance, event-detection accuracy, or comparison against an independent event-driven integrator. Because the central claim rests on quantitative differences between the two restitution maps, the absence of such verification leaves open the possibility that the reported attractor changes are sensitive to numerical implementation details.
Authors: We agree that additional numerical verification details will strengthen the paper. We will add a short subsection reporting the integration tolerances, event-detection thresholds for impacts, and direct comparisons of selected bifurcation and basin results against an independent event-driven integrator. These checks will demonstrate that the reported differences between the two restitution models are robust to implementation details. revision: yes
Circularity Check
No circularity: direct numerical comparison of two independent restitution models
full rationale
The paper formulates a hybrid non-smooth rocking-block model and performs direct numerical integration to generate bifurcation diagrams, Lyapunov exponents, and basins of attraction under two distinct restitution rules (Housner classical vs. Mao et al. alternative). No parameters are fitted from the target outputs, no predictions reduce to inputs by construction, and no self-citation chain or uniqueness theorem is invoked to justify the central comparison. The claimed differences in onset of complex oscillations and attractor properties follow from the explicit difference in the impact maps themselves, making the derivation self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Rocking-block motion is adequately described by a hybrid non-smooth system whose only non-smoothness is instantaneous impact governed by a scalar restitution coefficient.
Reference graph
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