1993
DOI: 10.1007/bf00375625
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On the dynamics of rods in the theory of Kirchhoff and Clebsch

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Cited by 138 publications
(109 citation statements)
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“…(1.5), which is 6 th order in the spatial derivatives of u. For a physical closed loop of wire with a small circular cross section of radius ρ > 0, a more realistic expression for the elastic potential energy is given by 16) where λ and µ are the Lamé constants for a homogeneous isotropic hyperelastic material (see [14]). (For a wire made of material of a fixed density, the kinetic energy is of order ρ 2 .…”
Section: Related Geometrical and Physical Problemsmentioning
confidence: 99%
See 2 more Smart Citations
“…(1.5), which is 6 th order in the spatial derivatives of u. For a physical closed loop of wire with a small circular cross section of radius ρ > 0, a more realistic expression for the elastic potential energy is given by 16) where λ and µ are the Lamé constants for a homogeneous isotropic hyperelastic material (see [14]). (For a wire made of material of a fixed density, the kinetic energy is of order ρ 2 .…”
Section: Related Geometrical and Physical Problemsmentioning
confidence: 99%
“…(1.14). Maddocks and Dichmann [15], Coleman et al [16] and others consider director theories, originated by Kirchhoff and Clebsch, in which there are further stress-strain relations between the tangent and two independent normal vectors (see [17]). The above choices for the potential and kinetic energy will not be pursued here.…”
Section: Related Geometrical and Physical Problemsmentioning
confidence: 99%
See 1 more Smart Citation
“…В работе [7] в замкну-той форме получены решения типа бегущих волн в линейно растяжимом и бесс-двиговом (тонком) плоском стержне. В работе [8] авторы представили описание нерастяжимых стержней с кручением и получили выражения для пространствен-ных (трехмерных) бегущих волн при наличии крутящего момента. В работе [9] обсуждается динамика изгиба плоского нерастяжимого стержня при условии пре-небрежения вращательной частью кинетической энергии, которая мала по сравне-нию с полной энергией стержня.…”
Section: Introductionunclassified
“…Сохранение импульса и углового момента и уравнения состояния (2.1) приводят к уравнениям для силы и момента [3], [8]:…”
Section: Introductionunclassified