@prefix this: . @prefix sub: . @prefix np: . @prefix rdf: . @prefix prov: . @prefix npx: . @prefix dc: . @prefix xsd: . sub:Head { this: a np:Nanopublication; np:hasAssertion sub:assertion; np:hasProvenance sub:provenance; np:hasPublicationInfo sub:pubinfo . } sub:assertion { a prov:SoftwareAgent; "delphisci dataset-resolvability assessor (Gemini 4 Argon)"; prov:actedOnBehalfOf ; . a ; dc: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."; dc:subject ; "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)."; "Gemini 4 Argon on buehler-2009-helical-networks-08: resolvable-now, resolvability 0.83"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0"; "The Inglis formula assumes an infinite, isotropic, homogeneous linear-elastic continuum under infinitesimal strain, which is only a heuristic approximation for a discrete, anisotropic, strongly nonlinear lattice at >100% strain."; "0.85"^^xsd:double; , ; "0.828"^^xsd:double; "resolvable-now" . a ; dc:isPartOf ; dc:subject ; "Analysis feasibility of buehler-2009-helical-networks-08 by Gemini 4 Argon: 0.9"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/analysis-feasibility"; "0.9"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Data adequacy of buehler-2009-helical-networks-08 by Gemini 4 Argon: 0.75"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/data-adequacy"; "0.75"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Data existence of buehler-2009-helical-networks-08 by Gemini 4 Argon: 0.85"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/data-existence"; "0.85"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Discriminating power of buehler-2009-helical-networks-08 by Gemini 4 Argon: 0.75"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/discriminating-power"; "0.75"^^xsd:double . a ; dc:isPartOf ; dc:subject ; "Operationalizability of buehler-2009-helical-networks-08 by Gemini 4 Argon: 0.9"; prov:wasAttributedTo ; "dataset-resolvability/0.2.0/operationalizability"; "0.9"^^xsd:double . , , , , , . a ; dc:description "open-access derivation and measured crack aspect ratios before and after yield-zone formation"; "Candidate dataset: Ackbarow et al. 2009 PLoS ONE Full Text and Parameter Table"; prov:wasDerivedFrom . a ; dc:description "open-source MD simulator to verify the undeformed and deformed crack aspect ratios in the 20-by-24 bead network"; "Candidate dataset: LAMMPS Molecular Dynamics Simulator"; prov:wasDerivedFrom . a ; dc:identifier "gemini-4-argon-medium"; "Gemini 4 Argon" . } sub:provenance { sub:assertion prov:wasAttributedTo ; prov:wasDerivedFrom , ; prov:wasGeneratedBy sub:assessment . sub:assessment a prov:Activity; prov:qualifiedAssociation sub:assessmentPlan; prov:wasAssociatedWith . sub:assessmentPlan prov:hadPlan . } sub:pubinfo { "buehler-protein-materials" . this: dc:created "2026-11-08T04:48:50.317Z"^^xsd:dateTime; dc:creator ; dc:license ; npx:hasNanopubType ; npx:introduces ; "Gemini 4 Argon on buehler-2009-helical-networks-08: resolvable-now, resolvability 0.83"; . sub:sig npx:hasAlgorithm "RSA"; npx:hasPublicKey "MIIBIjANBgkqhkiG9w0BAQEFAAOCAQ8AMIIBCgKCAQEAyFHtPB6p0mCjDozxlOY9CmO3nBm7Te3jFbXyLmM+G1tGe47Da0jYIbhkl9Oo1ZjxmCa3LCwlEqK8gj6hEIcL4ahW30JXh9HycfKVk1bugkzMEV15tJdTzAU3sGMFnbNsn43xY2LFLy45tApkRm5byEiM7oRRrooIdwoQKnP4Wzq/bfAoJ9qvW+MGkelyOTd1jbSt+KfmT7xKmDfWzAHddUlWwMX2QJOLxDaffOteTop6ZRgPiNmPJKA/S62Gac9XtSYT3oDkZ6/nr5cxxNLpOyxTf5FPISiCe11xYO/unYjY+mwnOfA8yhJIyx1l0O9I0vpOpn+E5TvyHJV+oSTrvwIDAQAB"; npx:hasSignature "TlETOO9/JYgY6SzZyOkUOdu2k/V9StwT/5c95pVrrF4ocNxlP9rV7Yx7O+FmFDJueJE/f9O5J04WsXaNDD8l19Y6A1Tez16uDB2BgIiA3/2l8uL2CUxTk5fj+/M1MquvknFkYsJRejjHm3BSAuJ8A/NNUufZJDbLCZkj/yabdgjwD3/Z1My/fHS+DiWFl+5v/eRDSVW1kPZvNHla3JeFjKOMMoM09kAr77Mz7RKwDbbQJtCANDb56EgVB/Kj7+/rnRuHpwyjNa/+J+VH2HTZrDUWncEVsett+SJv+Da/d92Nw1e+3TXOOJSRXyMDAhceT71Ch9DGnfsJ3M3c7B79fA=="; npx:hasSignatureTarget this:; npx:signedBy . }