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Lie symmetry theorem of fractional nonholonomic systems 被引量:3
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作者 孙毅 陈本永 傅景礼 《Chinese Physics B》 SCIE EI CAS CSCD 2014年第11期111-117,共7页
The Lie symmetry theorem of fractional nonholonomic systems in terms of combined fractional derivatives is estab- lished, and the fractional Lagrange equations are obtained by virtue of the d'Alembert-Lagrange princi... The Lie symmetry theorem of fractional nonholonomic systems in terms of combined fractional derivatives is estab- lished, and the fractional Lagrange equations are obtained by virtue of the d'Alembert-Lagrange principle with fractional derivatives. As the Lie symmetry theorem is based on the invariance of differential equations under infinitesimal trans- formations, by introducing the differential operator of infinitesimal generators, the determining equations are obtained. Furthermore, the limit equations, the additional restriction equations, the structural equations, and the conserved quantity of Lie symmetry are acquired. An example is presented to illustrate the application of results. 展开更多
关键词 Lie symmetry conserved quantity fractional nonholonomic systems
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Symplectic-energy-first integrators of discrete mechanico-electrical dynamical systems 被引量:1
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作者 傅景礼 陈本永 +1 位作者 唐贻发 付昊 《Chinese Physics B》 SCIE EI CAS CSCD 2008年第11期3942-3952,共11页
A discrete total variation calculus with variable time steps is presented for mechanico-electrical systems where there exist non-potential and dissipative forces. By using this discrete variation calculus, the symplec... A discrete total variation calculus with variable time steps is presented for mechanico-electrical systems where there exist non-potential and dissipative forces. By using this discrete variation calculus, the symplectic-energy-first integrators for mechanico-electrical systems are derived. To do this, the time step adaptation is employed. The discrete variational principle and the Euler-Lagrange equation are derived for the systems. By using this discrete algorithm it is shown that mechanico-electrical systems are not symplectic and their energies are not conserved unless they are Lagrange mechanico-electrical systems. A practical example is presented to illustrate these results. 展开更多
关键词 total variation symplectic-energy-momentum integrator mechanico-electrical system
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