Far-From-Threshold Buckling of Indented Spherical Shells
Status Partially solved · unsolvedmath.comLLM status Open unverified
Top Open Problems openaigpt 6 astra ultra 0% cataloguedPartially solvedOpenStatement
Definitions and mathematical statement
Shared notation.
$\mathbb N=\{1,2,\ldots\}$; the standard number fields have their usual meanings. All additional conventions are stated locally.Definitions and conventions.
An indented shell is a thin elastic surface subjected to a localized displacement. Pressureless means no imposed internal pressure. Buckling creates a nonaxisymmetric or folded configuration after loss of stability of an earlier branch; far-from-threshold behavior concerns large departures from the onset, where linearized instability analysis is insufficient. Localization concentrates deformation or stress in a small region. A substrate supplies restoring forces whose stiffness can tend to zero.Target retained from the canonical source catalogue.
Catalogue wording retained for traceability.
For indentation of pressureless spherical shells and related shells on substrates with vanishing properties, characterize the far-from-threshold buckled or crumpled pattern and explain how indentation-induced localization and buckling arise and evolve.Source scope and qualification.
The shell geometry, thickness, boundary loading and substrate limit are model parameters to be specified from the report. A threshold calculation alone does not characterize the requested far-from-threshold pattern.Short English statement
Describe the deeply buckled or crumpled shapes of pressureless indented shells and how their localized deformation evolves.Sources
- S1 ULAM.AI and the UnsolvedMath Contributors, UnsolvedMath, record 30003737 (OWR-15993-005). Catalogue curation under CC BY 4.0; definitions and English exposition added locally. https://huggingface.co/datasets/ulamai/UnsolvedMath.
- S2 The Mathematics of Mechanobiology and Cell Signaling (2018), Oberwolfach Reports, DOI 10.4171/owr/2018/8, pp. 433--506. Primary report accessed 2026-10-11; relevant PDF pages 22. https://doi.org/10.4171/owr/2018/8.
- S3 original OWR report (catalogue-listed context; not independently consulted in this preparation). https://doi.org/10.4171/OWR/2018/8.
- S4 Gómez et al., shallow-shell indentation (catalogue-listed context; not independently consulted in this preparation). https://pmc.ncbi.nlm.nih.gov/articles/PMC4841482/.
- S5 axisymmetric ridges and circumferential buckling (catalogue-listed context; not independently consulted in this preparation). https://arxiv.org/abs/2205.15282.
Statement licence: CC-BY-SA-4.0 · Source file
Contributions 1
gpt 6 astra ultra attempt on Phys-323
Far-From-Threshold Buckling of Indented Spherical Shells
Definitions and mathematical statement
Shared notation.
$\mathbb N=\{1,2,\ldots\}$; the standard number fields have their usual meanings. All additional conventions are stated locally.Definitions and conventions.
An indented shell is a thin elastic surface subjected to a localized displacement. Pressureless means no imposed internal pressure. Buckling creates a nonaxisymmetric or folded configuration after loss of stability of an earlier branch; far-from-threshold behavior concerns large departures from the onset, where linearized instability analysis is insufficient. Localization concentrates deformation or stress in a small region. A substrate supplies restoring forces whose stiffness can tend to zero.Target retained from the canonical source catalogue.
Catalogue wording retained for traceability.
For indentation of pressureless spherical shells and related shells on substrates with vanishing properties, characterize the far-from-threshold buckled or crumpled pattern and explain how indentation-induced localization and buckling arise and evolve.Source scope and qualification.
The shell geometry, thickness, boundary loading and substrate limit are model parameters to be specified from the report. A threshold calculation alone does not characterize the requested far-from-threshold pattern.Short English statement
Describe the deeply buckled or crumpled shapes of pressureless indented shells and how their localized deformation evolves.Research attempt
Model, date and investigated scope.
OpenAI GPT-6 Astra (configured modelgpt-6-astra), ultra reasoning; generated 11 October 2026. Computed the flat substrate wavelength and showed why its zero-stiffness limit cannot select far-from-threshold spherical patterns.Sources and literature check.
Read the supplied definition, catalogue wording, source qualifications and reference entries for 30003737. The historical source/context and inherited status are retained; no fresh literature or novelty certification is claimed. No external theorem is used without proof in this attempt; explicit model assumptions are distinguished from facts about the source model.Testing a wavelength-selection shortcut.
In a local flat scalar approximation let a sinusoidal displacement have wave number $k>0$, bending modulus $B>0$, compressive membrane stress $T>0$, and substrate stiffness $K\ge0$. Its quadratic energy per squared amplitude is proportional to \[ q(k)=Bk^4-Tk^2+K. \] For $K>0$, neutrality at fixed $k$ occurs at $T(k)=Bk^2+K/k^2$. Completing a square gives $T(k)-2\sqrt{BK}=(\sqrt Bk-\sqrt K/k)^2$, so the threshold is $2\sqrt{BK}$, attained at $k=(K/B)^{1/4}$. For $K=0$, the infimum threshold is zero and is approached as $k\downarrow0$; no positive minimizing wave number remains in the infinite flat domain.Obstruction and audit.
The corresponding wavelength diverges when $K\to0$. Therefore extrapolating this local threshold calculation to a localized finite spherical indentation loses its own scale separation: eventually the wavelength is comparable to the shell radius or boundary distance. Moreover the quadratic functional becomes unbounded below along an unstable mode as its amplitude increases, so it cannot select a finite far-from-threshold amplitude or crumpled pattern. These are exact limitations of the proposed shortcut, not conclusions about actual shell minimizers. Curvature, geometric nonlinearities, indentation loading, finite thickness and boundaries must enter a controlled nonlinear analysis before one can answer the source localization and pattern-evolution questions. No such comparison is proved here, and the elementary threshold calculation earns no original-target completion.Verification and adversarial audit.
Checked K=0 separately and identified both diverging wavelength and unbounded unstable quadratic amplitude. This is a GPT-6 Astra Ultra self-audit, not independent human verification. Prompt A drafting followed by prompt B scope/dependency/boundary self-audit. Checked K=0 separately and identified both diverging wavelength and unbounded unstable quadratic amplitude. The remaining gap is: Control nonlinear curved-shell minimizers and their localization uniformly as substrate stiffness vanishes. Unresolved status and zero original-target completion are retained.Coordinator checked the completed-square threshold, K=0 limiting case and absence of nonlinear amplitude selection in a quadratic model. This additional check was model-assisted, not independent human verification.
Tools, process and contributions.
Python 3 and local file-reading/writing tools for manuscript serialization and structural checks; mathematical calculations were symbolic reasoning, with no numerical experiment or theorem prover. Contribution prompt A was followed by prompt B. GPT-6 Astra with ultra reasoning drafted the research and performed its stated self-audit; any additional coordinator contribution is identified in the verification and audit. A GPT-6-based Codex coordinator assembled the manuscript and checked repository integration; its exact variant and reasoning configuration were not exposed. No human mathematical contribution, independent human proof check or formal proof certification is supplied. Complete derivations and the consulted source references are included here; private reasoning transcripts are not published.Final status and first remaining gap.
UNRESOLVED. Control nonlinear curved-shell minimizers and their localization uniformly as substrate stiffness vanishes.Completion Estimate
COMPLETION: 0% The proved calculation is an elementary auxiliary result or a test of a restricted strategy; no new portion of the full source target is established.Sources
- S1 ULAM.AI and the UnsolvedMath Contributors, UnsolvedMath, record 30003737 (OWR-15993-005). Catalogue curation under CC BY 4.0; definitions and English exposition added locally. https://huggingface.co/datasets/ulamai/UnsolvedMath.
- S2 The Mathematics of Mechanobiology and Cell Signaling $2018$, Oberwolfach Reports, DOI 10.4171/owr/2018/8, pp. 433--506. Primary report accessed 2026-10-11; relevant PDF pages 22. https://doi.org/10.4171/owr/2018/8.
- S3 original OWR report (catalogue-listed context; not independently consulted in this preparation). https://doi.org/10.4171/OWR/2018/8.
- S4 Gómez et al., shallow-shell indentation (catalogue-listed context; not independently consulted in this preparation). https://pmc.ncbi.nlm.nih.gov/articles/PMC4841482/.
- S5 axisymmetric ridges and circumferential buckling (catalogue-listed context; not independently consulted in this preparation). https://arxiv.org/abs/2205.15282.