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The first method Yuryev force generation and / or moments within the closed VARIABLE multibody system for its linear and / or angular displacements in space without interaction with the environment AND DEVICE FOR ITS IMPLEMENTATION
The first method Yuryev force generation and / or moments within the closed VARIABLE multibody system for its linear and / or angular displacements in space without interaction with the environment AND DEVICE FOR ITS IMPLEMENTATION
1. A first method of forming Yureva forces and / or moments within the closed system for variable miogomassovoy its linear and / or angular movement in space without any interaction with the external environment, the total mass m which is able to generate and accumulate the energy increment and comprises a passive mass moving relative thereto MI active compositions, comprising: from 4 · n nondeformable coaxial pairs of mass mc cylindrical relatively rotating surfaces common to each of these pairs of masses axes of rotation, where n - the number of pairs 2 · p poles pformi tion of internal forces influence on the total weight of m systems, j = 1, 2, ..., 2 · n - pole sequence number forming the internal forces of impact on the total mass m of the system, i = 0, 1, 2, ..., 9 - number of physical value at a pole; and, if necessary, of 4 · n elastically deformable masses mrekuperatsii increments kinetic energy of rotational movement of the masses MW of each of the pair relative to one another - based on the fact that between pairs of non-deformable coaxial pairs m masses belonging to the same p pole form linkages so that their rotation axis is always interconnected and are movable in opposite directions relative to each other parallel directions of translational movement orthogonal to the directions of their axes of rotation, and each of nedeform iruemyh mass coaxial pair, if necessary, is interconnected with another deformable mass of the same pair through a coaxial resiliently deformable mass of m, a middle portion which is fixed relative to the direction of translational motion of the axis of rotation of the pair of coaxial nondeformable mass m, is then set at neobhodimos
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