2006
DOI: 10.1007/s00158-005-0601-6
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Michell cantilevers constructed within trapezoidal domains—Part III: force fields

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Cited by 18 publications
(10 citation statements)
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“…Complementary to region T 4 , there will need to be two additional regions T 5 and T 5 , sim- (Pichugin et al 2012) ilar to, but not identical to the fields constructed by Chan (1967) (H. S. Y. Chan's solutions assume that the vertical boundaries of the domain are fixed, whereas in our case one must enforce the conditions for reflective symmetry). One can then construct further extensions of the field above, by adding further fully strained regions akin to the approach taken for Michell cantilevers by Lewiński et al (1994), Graczykowski and Lewiński (2006a), Graczykowski and Lewiński (2006b), and Graczykowski and Lewiński (2007).…”
Section: Global Optimalitymentioning
confidence: 99%
“…Complementary to region T 4 , there will need to be two additional regions T 5 and T 5 , sim- (Pichugin et al 2012) ilar to, but not identical to the fields constructed by Chan (1967) (H. S. Y. Chan's solutions assume that the vertical boundaries of the domain are fixed, whereas in our case one must enforce the conditions for reflective symmetry). One can then construct further extensions of the field above, by adding further fully strained regions akin to the approach taken for Michell cantilevers by Lewiński et al (1994), Graczykowski and Lewiński (2006a), Graczykowski and Lewiński (2006b), and Graczykowski and Lewiński (2007).…”
Section: Global Optimalitymentioning
confidence: 99%
“…Having found these axial forces (which are constant along the boundary lines DB, DC) one can solve the equilibrium problem of the interior of the domain ABDC, i.e. find the internal forces in the meaning of Hemp (1973) by following the method developed in Graczykowski and Lewiński (2007a). These internal forces are defined by…”
Section: Geometry Of the Domain Rbdcnarmentioning
confidence: 99%
“…The desired final material distribution contains two distinct regions of fully dense material (ρ = 1) and regions that have zero relative density (ρ min <<1) with the fully dense regions representing the optimized topology. The final material distribution can be described by the probability distribution function, f f , given by (14) and the corresponding final cumulative distribution is given by (15) A gradual transition from the initial distribution to the final distribution can be achieved through the use of the beta function (17) where Γ is the gamma function. The corresponding cumulative distribution function, also known as the incomplete beta function, is given by …”
Section: Prescribed Materials Redistribution Methodsmentioning
confidence: 99%
“…Following the initial pioneering work of Michell [1] and a flourish of advances in the 1950's and 1960's (Cox [2]; Hemp [3]; Prager [4]; Chan [5]), the analysis of absolute minimum-weight truss structures entered a period of relative neglect until the 1990's since when it has become a subject of renewed interest; see for example the work by Rozvany et al [6][7][8]; Lewinski et al [9]; Lewinski and Rozvany [10][11][12]; Graczykowski and Lewinski [13][14][15]; Dewhurst [16,17]; Dewhurst and Srithongchai [18]; Srithongchai and Dewhurst [19]; Dewhurst et al [20].…”
Section: Introductionmentioning
confidence: 99%