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6 Feb 2014: Table 2Calculations of characters for representations in the 3D symmetry-extended Maxwell Eq. ... To preserve the Maxwell count, each additional joint isaccompanied by 3 new bars.

7 Aug 2014: Maxwell’s 1864 rule for pin-jointed frameworks [1], in the extension due to Calladine [2] is. ... References. 1. Maxwell, J.C. On the calculation of the equilibrium and stiffness of frames.

6 Feb 2014: In 1864, James Clerk Maxwell identified a simplecounting condition that must hold if an idealized bar-joint structure is to be rigid to first order.

6 Feb 2014: translation.Thus, the symmetry-extended Maxwell rule (5.5) gives a complete solution in this case. ... References1. Maxwell JC. 1864 On the calculation of the equilibrium and stiffness of frames.

6 Feb 2014: PACS 62.20.dj – Poisson’s ratio. Abstract – A symmetry-extended Maxwell treatment of the net mobility of periodic bar-and-joint frameworks is used to derive a sufficient condition for ... 34] Calladine C. R., Int. J. Solids Struct., 14 (1978)

7 Aug 2014: same way as Calladine’s extension (Calladine, 1978) of Maxwell’s Rule for. ... bar-and-joint frameworks (Maxwell, 1864) is. ms = 6(b 1) 6g gi=1.

6 Feb 2014: These finite pin-jointed structures have beenextensively studied. Maxwell (1864) introduced a simple rule: a system having jjoints and no kinematic constraints requires at least 3j 6 (in three dimensions)or ... J. Eng. Math. 4,

6 Feb 2014: R. 1978 Buckminster Fuller’s “tensegrity” structures and Clerk Maxwell’s rules for. ... D. 2000 A symmetry extension of Maxwell’s rule for rigidity of frames.

6 Feb 2014: Guest (2000) to establish the symmetry-extended version of Maxwell’s rule for bar and joint frameworks(see also Schulze, in press-b, for further details). ... Fowler, P.W., Guest, S.D., 2000. A symmetry extension of Maxwell’s rule for rigidityof

6 Feb 2014: The same symmetry has been derived for the states of self-stress of toroidaldeltahedra using symmetry-extended Maxwell analysis (Fowler & Guest 2002),and occurs as a contribution to the mobility equation