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Symmetry elements second-order applications

In Equation (4.12) the discretization of velocity and pressure is based on different shape functions (i.e. NjJ = l,n and Mil= l,m where, in general, mweight function used in the continuity equation is selected as -Mi to retain the symmetry of the discretized equations. After application of Green s theorem to the second-order velocity derivatives (to reduce inter-element continuity requirement) and the pressure terms (to maintain the consistency of the formulation) and algebraic manipulations the working equations of the U-V-P scheme are obtained as... [Pg.114]

The notation of the symmetry center or inversion center is 1 while the corresponding combined application of twofold rotation and mirror-reflection may also be considered to be just one symmetry transformation. The symmetry element is called a mirror-rotation symmetry axis of the second order, or twofold mirror-rotation symmetry axis and it is labeled 2. Thus, 1 = 2. [Pg.55]

In polymers XVII and XVIII, the second-order polar axis directed along the layers and perpendicular to the plane of the slope of the chiral fiagments is the only symmetry element. On application of an electric field along this axis. [Pg.229]


See other pages where Symmetry elements second-order applications is mentioned: [Pg.109]    [Pg.526]    [Pg.174]    [Pg.174]    [Pg.331]    [Pg.220]    [Pg.71]    [Pg.182]    [Pg.175]    [Pg.35]    [Pg.170]    [Pg.19]    [Pg.199]    [Pg.67]    [Pg.228]    [Pg.351]    [Pg.320]    [Pg.442]    [Pg.394]   
See also in sourсe #XX -- [ Pg.563 , Pg.564 , Pg.565 ]




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Elements: applications

Second-order applications

Second-order element

Symmetry applications

Symmetry elements

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