Equilibrium and absolute minimal states of Mumford-Shah functionals and brittle fracture pr.pdf
- 1、本文档共23页,可阅读全部内容。
- 2、有哪些信誉好的足球投注网站(book118)网站文档一经付费(服务费),不意味着购买了该文档的版权,仅供个人/单位学习、研究之用,不得用于商业用途,未经授权,严禁复制、发行、汇编、翻译或者网络传播等,侵权必究。
- 3、本站所有内容均由合作方或网友上传,本站不对文档的完整性、权威性及其观点立场正确性做任何保证或承诺!文档内容仅供研究参考,付费前请自行鉴别。如您付费,意味着您自己接受本站规则且自行承担风险,本站不退款、不进行额外附加服务;查看《如何避免下载的几个坑》。如果您已付费下载过本站文档,您可以点击 这里二次下载。
- 4、如文档侵犯商业秘密、侵犯著作权、侵犯人身权等,请点击“版权申诉”(推荐),也可以打举报电话:400-050-0827(电话支持时间:9:00-18:30)。
查看更多
Equilibrium and absolute minimal states of Mumford-Shah functionals and brittle fracture pr
a
r
X
i
v
:
0
7
0
4
.2
6
8
7
v
2
[
m
a
t
h
.A
P
]
1
4
M
a
r
2
0
0
8
Equilibrium and absolute minimal states of Mumford-Shah
functionals and brittle fracture propagation
Marius Buliga?
Abstract
By a combination of geometrical and configurational analysis we study the
properties of absolute minimal and equilibrium states of general Mumford-Shah
functionals, with applications to models of quasistatic brittle fracture propagation.
The main results concern the mathematical relations between physical quantities
as energy release rate and energy concentration for 3D cracks with complex shapes,
seen as outer measures living on the crack edge.
Keywords: 3D brittle fracture; energy methods; Mumford-Shah functional
1 Introduction
A new direction of research in brittle fracture mechanics begins with the article of
Mumford Shah [12] regarding the problem of image segmentation. This problem,
which consists in finding the set of edges of a picture and constructing a smoothed
version of that picture, it turns to be intimately related to the problem of brittle crack
evolution. In the before mentioned article Mumford and Shah propose the following
variational approach to the problem of image segmentation: let g : ? ? R2 → [0, 1] be
the original picture, given as a distribution of grey levels (1 is white and 0 is black), let
u : ? → R be the smoothed picture and K be the set of edges. K represents the set
where u has jumps, i.e. u ∈ C1(? \K,R). The pair formed by the smoothed picture u
and the set of edges K minimizes then the functional:
I(u,K) =
∫
?
α | ?u |2 dx +
∫
?
β | u? g |2 dx + γH1(K) .
The parameter α controls the smoothness of the new picture u, β controls the L2
distance between the smoothed picture and the original one and γ controls the total
length of the edges given by this variational method. The authors remark that for β = 0
the functional I might be useful for an energetic treatment of fracture mechanics.
An energetic approach to fracture mechanics is natur
您可能关注的文档
- DEAR BENJAMIN.ppt
- Dear Alumni, Management Internship Program - Batch I.pdf.pdf
- Dear friend.ppt
- Dear purchasing manager.doc
- Dear Colleagues, Message from the Editors-in-Chief.pdf
- Dear students.ppt
- Dear ________________ APPENDIX C PERMISSION LETTER TO STUDY SITE.pdf
- Decoherence at absolute zero.pdf
- Decoherence for phase-sensitive relaxation.pdf
- Deformed Chern-Simons interaction for nonrelativistic point particles.pdf
文档评论(0)