Skip to content
DraconiticResearch
Search Sources API
201,642 studies31 sourcesUpdated 13 min ago
PreprintarXiv licencearXiv

The hypoexponential form for the fiber-length distribution in thermoplastic composites revisited: finite initial length, cascade fracture, and its mechanistic status

Abstract

In a previous work [Masubuchi et al., Compos. Sci. Technol. 134, 43 (2016)], a fiber-length distribution function was proposed as the hypoexponential, or Erlang-type, convolution of two exponential waiting lengths, motivated by two independent Poisson processes for breakage and for blocking of adjacent breaks. The present paper further evaluates this hypoexponential form by introducing a finite initial length L_{0}, and by analyzing the mechanistic basis of the buckling-induced fiber breakage process. The obtained finite-L_{0} closed-form solution was compared to a glass fiber dataset to retroactively justify the infinite-length idealization in the earlier work for such systems while providing the complete form for processes in which fragments remain comparable to L_{0}. Concerning the mechanics of fiber fragmentation, a Mellin transform analysis of the fragmentation equation showed that scale-invariant cascades yield power laws and therefore cannot generate characteristic lengths; those lengths must instead arise from scale-breaking ingredients, particularly the cutoff region and the arrested processing history. Monte Carlo simulations of a phenomenological finite-opportunity cascade showed that the hypoexponential form does not reproduce the peak of the generated distribution but captures its exponential-like tail, implying that it serves as a useful two-parameter fitting model, although not an exact generative distribution.

Related

  1. Continuous in-situ synchrotron micro-XCT observation of thermoplastic composite laminate consolidation
    Adrien Le Reun, Nicolas Lefevre, Henri-Alexandre Cayzac +3
    Composites Part B: EngineeringPeer-reviewedCC BY-NC-SA 4.0Full text2 citedApplied physics & instrumentationHAL
  2. Thermoplastic Dielectric Coatings for Flexible Electrodynamic Dust Shields: Structural and Functional Performance
    Ide E. Onal, Emily A. Ryan, Luca Scifoni +4
    Advanced Materials InterfacesPeer-reviewedCC BYFull textGeneral physicsDOAJ
  3. The Longest Increasing Subsequence Problem revisited
    Silvio Franz, Roberto Mulet
    Communications in Theoretical PhysicsPeer-reviewedLicence not statedGeneral physicsHAL
  4. Silica fibers as spontaneous four-wave mixing sources of photon pairs: Raman noise revisited
    Philippe Delaye
    Optics LettersPeer-reviewedPublisher termsFull textOptics & photonicsQuantum physics & quantum informationHAL
  5. Revisited String Theory
    Alaya Kouki
    Current Research in Traffic Transportation EngineeringPeer-reviewedCC BYFull textGeneral physicsHAL
BibTeX
@misc{masubuchi2026hypoexponential,
  title = {{The hypoexponential form for the fiber-length distribution in thermoplastic composites revisited: finite initial length, cascade fracture, and its mechanistic status}},
  author = {Yuichi Masubuchi},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.20312},
  eprint = {2609.20312},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.20312},
}
RIS
TY  - UNPB
TI  - The hypoexponential form for the fiber-length distribution in thermoplastic composites revisited: finite initial length, cascade fracture, and its mechanistic status
AU  - Yuichi Masubuchi
PY  - 2026
DA  - 2026/09/01
PB  - arXiv
DO  - 10.48550/arxiv.2609.20312
UR  - https://arxiv.org/abs/2609.20312
AB  - In a previous work [Masubuchi et al., Compos. Sci. Technol. 134, 43 (2016)], a fiber-length distribution function was proposed as the hypoexponential, or Erlang-type, convolution of two exponential waiting lengths, motivated by two independent Poisson processes for breakage and for blocking of adjacent breaks. The present paper further evaluates this hypoexponential form by introducing a finite initial length L_{0}, and by analyzing the mechanistic basis of the buckling-induced fiber breakage process. The obtained finite-L_{0} closed-form solution was compared to a glass fiber dataset to retroactively justify the infinite-length idealization in the earlier work for such systems while providing the complete form for processes in which fragments remain comparable to L_{0}. Concerning the mechanics of fiber fragmentation, a Mellin transform analysis of the fragmentation equation showed that scale-invariant cascades yield power laws and therefore cannot generate characteristic lengths; those lengths must instead arise from scale-breaking ingredients, particularly the cutoff region and the arrested processing history. Monte Carlo simulations of a phenomenological finite-opportunity cascade showed that the hypoexponential form does not reproduce the peak of the generated distribution but captures its exponential-like tail, implying that it serves as a useful two-parameter fitting model, although not an exact generative distribution.
ER  -