https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY/Head https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY http://www.nanopub.org/nschema#hasAssertion https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY/assertion https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY http://www.nanopub.org/nschema#hasProvenance https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY/provenance https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY http://www.nanopub.org/nschema#hasPublicationInfo https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY/pubinfo https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY http://www.w3.org/1999/02/22-rdf-syntax-ns#type http://www.nanopub.org/nschema#Nanopublication https://w3id.org/np/RAe58o0xKQPsd6j5wDwzJOfRdj6a1ifWUV-VbOFUZqmrY/assertion https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium http://www.w3.org/1999/02/22-rdf-syntax-ns#type http://www.w3.org/ns/prov#SoftwareAgent https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium http://www.w3.org/2000/01/rdf-schema#label delphisci dataset-resolvability assessor (Gemini 4 Argon) https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium http://www.w3.org/ns/prov#actedOnBehalfOf https://orcid.org/0009-0007-4948-9192 https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium https://w3id.org/delphi/ontology/usesModel https://w3id.org/delphi/resource/model/gemini-4-argon-medium https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini http://purl.org/dc/terms/description As stated, the claim applies the analytical Inglis formula to the crack aspect ratios before (a_0/b_0 = 3, giving magnification 7.0) and after (a_1/b_1 = 0.11, giving magnification 1.22) yield-zone formation, which immediately yields 7.0 / 1.22 = 5.74 ≈ 5.7. Furthermore, the aspect-ratio change itself can be directly reproduced by running the open-access LAMMPS bead model. While the continuum Inglis solution is an idealized approximation for a discrete nonlinear network, the mathematical calculation and simulated geometry are both checkable now. https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini http://purl.org/dc/terms/subject https://w3id.org/delphi/resource/concept/dataset-resolvability-0.2.0 https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini http://www.w3.org/1999/02/22-rdf-syntax-ns#type https://w3id.org/delphi/ontology/LLMClaimAssessment https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini http://www.w3.org/2000/01/rdf-schema#comment Proposed test with existing data: Substitute the initial crack aspect ratio (a_0 / b_0 = 3) and the post-yield transformed aspect ratio (a_1 / b_1 = 0.11) measured from the mesoscale network simulation into the Inglis elliptical hole formula sigma_tip = sigma_inf (1 + 2 a / b), and verify both the aspect ratios in LAMMPS and that the predicted stress magnification factor drops from 7.0 to 1.22 (a factor of 5.7). https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini http://www.w3.org/2000/01/rdf-schema#label Gemini 4 Argon on buehler-2009-helical-networks-08: resolvable-now, resolvability 0.83 https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini http://www.w3.org/ns/prov#wasAttributedTo https://w3id.org/delphi/resource/agent/delphisci-resolvability-assessor-gemini-4-argon-medium https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini https://w3id.org/delphi/ontology/assessmentType dataset-resolvability/0.2.0 https://w3id.org/delphi/resource/assessment/buehler-2009-helical-networks-08--gemini https://w3id.org/delphi/ontology/evidenceAgainst The Inglis formula assumes an infinite, isotropic, homogeneous linear-elastic continuum under infinitesimal strain, which is only a heuristic approximation for a discrete, 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