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− | ==1 Title, abstract and keywords<!-- Your document should start with a concise and informative title. Titles are often used in information-retrieval systems. Avoid abbreviations and formulae where possible. Capitalize the first word of the title. | + | ==Abstract== |
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− | Provide a maximum of 6 keywords, and avoiding general and plural terms and multiple concepts (avoid, for example, 'and', 'of'). Be sparing with abbreviations: only abbreviations firmly established in the field should be used. These keywords will be used for indexing purposes.
| + | This paper reviews briefly the formulations used over the last 40 |
| + | years for the solution of problems involving tensile cracking, both with |
| + | the discrete and smeared crack approaches. The paper focuses in the |
| + | smeared approach, identifying as its main drawbacks the observed |
| + | mesh-size and mesh-bias spurious dependence when the method is |
| + | applied “straightly”. A simple isotropic local damage constitutive |
| + | model is considered, and the (exponential) softening modulus is regularized |
| + | according to the material fracture energy and the element |
| + | size. The continuum and discrete mechanical problems corresponding |
| + | to both the weak discontinuity (smeared cracks) and strong discontinuity |
| + | (discrete cracks) approaches are analyzed and the question of |
| + | propagation of the strain localization band (crack) is identified as the |
| + | main difficulty to be overcome in the numerical procedure. A tracking |
| + | technique is used to ensure uniqueness of the solution, attaining the |
| + | necessary stability and convergence properties of the corresponding |
| + | discrete finite element formulation. Numerical examples show that the |
| + | formulation derived is well posed, stable and remarkably robust. As |
| + | a consequence, the results obtained do not suffer from spurious meshsize |
| + | or mesh-bias dependence, comparing very favorably with those |
| + | obtained with other fracture and continuum mechanics approaches. |
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− | An abstract is required for every document; it should succinctly summarize the reason for the work, the main findings, and the conclusions of the study. Abstract is often presented separately from the article, so it must be able to stand alone. For this reason, references and hyperlinks should be avoided. If references are essential, then cite the author(s) and year(s). Also, non-standard or uncommon abbreviations should be avoided, but if essential they must be defined at their first mention in the abstract itself. -->==
| + | <pdf>Media:Draft_Samper_811836495_6794_Pl295.pdf</pdf> |
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− | ==2 The main text<!-- You can enter and format the text of this document by selecting the ‘Edit’ option in the menu at the top of this frame or next to the title of every section of the document. This will give access to the visual editor. Alternatively, you can edit the source of this document (Wiki markup format) by selecting the ‘Edit source’ option.
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− | 2.1 Subsections
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− | Divide your article into clearly defined and numbered sections. Subsections should be numbered 1.1, 1.2, etc. and then 1.1.1, 1.1.2, ... Use this numbering also for internal cross-referencing: do not just refer to 'the text'. Any subsection may be given a brief heading. Capitalize the first word of the headings.
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− | 2.2 General guidelines
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− | 1. The first entry in this list
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− | You may choose to number equations for easy referencing. In that case they must be numbered consecutively with Arabic numerals in parentheses on the right hand side of the page. Below is an example of formulae that should be referenced as eq. (1].
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− | 2.4 Supplementary material
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− | Supplementary material can be inserted to support and enhance your article. This includes video material, animation sequences, background datasets, computational models, sound clips and more. In order to ensure that your material is directly usable, please provide the files with a preferred maximum size of 50 MB. Please supply a concise and descriptive caption for each file. -->==
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− | ==3 Bibliography<!--
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− | ==4 Acknowledgments<!-- Acknowledgments should be inserted at the end of the document, before the references section. -->==
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− | ==5 References<!--[1] Author, A. and Author, B. (Year) Title of the article. Title of the Publication. Article code. Available: http://www.scipedia.com/ucode.
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− | [2] Author, A. and Author, B. (Year) Title of the article. Title of the Publication. Volume number, first page-last page.
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− | [3] Author, C. (Year). Title of work: Subtitle (edition.). Volume(s). Place of publication: Publisher.
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− | [4] Author of Part, D. (Year). Title of chapter or part. In A. Editor & B. Editor (Eds.), Title: Subtitle of book (edition, inclusive page numbers). Place of publication: Publisher.
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− | [5] Author, E. (Year, Month date). Title of the article. In A. Editor, B. Editor, and C. Editor. Title of published proceedings. Paper presented at title of conference, Volume number, first page-last page. Place of publication.
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− | [6] Institution or author. Title of the document. Year. [Online] (Date consulted: day, month and year). Available: http://www.scipedia.com/document.pdf.
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This paper reviews briefly the formulations used over the last 40
years for the solution of problems involving tensile cracking, both with
the discrete and smeared crack approaches. The paper focuses in the
smeared approach, identifying as its main drawbacks the observed
mesh-size and mesh-bias spurious dependence when the method is
applied “straightly”. A simple isotropic local damage constitutive
model is considered, and the (exponential) softening modulus is regularized
according to the material fracture energy and the element
size. The continuum and discrete mechanical problems corresponding
to both the weak discontinuity (smeared cracks) and strong discontinuity
(discrete cracks) approaches are analyzed and the question of
propagation of the strain localization band (crack) is identified as the
main difficulty to be overcome in the numerical procedure. A tracking
technique is used to ensure uniqueness of the solution, attaining the
necessary stability and convergence properties of the corresponding
discrete finite element formulation. Numerical examples show that the
formulation derived is well posed, stable and remarkably robust. As
a consequence, the results obtained do not suffer from spurious meshsize
or mesh-bias dependence, comparing very favorably with those
obtained with other fracture and continuum mechanics approaches.