Patent UA-78589-U (UA)
Title: Method for transformation of forces of inertia to driving force
Inventor: CHUHUI VOLODYMYR LEONIDOVYCH
IPC: F03G3/08
Filed: 2012-09-10
Abstract: A method for converting of inertia forces to driving force in which two loads are installed each at its own link, each link is connected to its individual shaft, two shafts are parallel to each other, at the tip of each shaft an individual cylindrical toothed pinion is installed. Teeth of two pinions are engaged one with another, there one of individual shafts is rotated, through the toothed pinions rotation is transferred to the other shaft, as the result two shafts are rotated together with links and loads with same angular velocity in opposite directions in counter-phase as to the plane of symmetry of two shafts, and as result of rotation of the loads normal inertia forces directed in radial direction act on the loads, vector sum of those is obtained as a directed vector of inertia forces, line of action of that goes through the line of symmetry of two loads, and the value of the vector of resultant inertia forces is harmonically changed. Bearings of the shafts are installed on the frame connected to eccentric journal of the eccentric shaft, the teeth of one of the pinions are engaged with the teeth of the wheel installed at the section of the eccentric journal placed out of the section between two jaws of the eccentric shaft, and for converting to rotary forces (traction) the frame is hinged on the eccentric journal of the eccentric shaft and is hinged on the eccentric journal of the second eccentric shaft, and the wheel is fixed on the eccentric journal of the eccentric shaft, and for t converting to moving forces (traction) the frame is fixed on eccentric journal of the eccentric shaft, and the wheel is fit with capability of rotation to the eccentric journal of the eccentric shaft, and the hub of the wheel is connected to the hub of the second wheel fit to that eccentric journal of the eccentric shaft, and the teeth of the second wheel are engaged to the teeth of the third wheel fit with capability of rotation to the main journal of the eccentric shaft, and the third wheel is braked, there one rotates the eccentric shaft with respect to the axis of its main journals and through the toothed wheel and the pinions rotation of the eccentric shaft is transferred to the shafts and the links with loads on the frame, and from motion of the loads one obtains directed inertia forces, and at converting to rotary forces (traction) at rotation of the eccentric shaft the line of effect of resultant inertia forces is in plane-parallel way displaced in circle with respect to the axis of rotation of the eccentric shaft, with motion of the line of effect of inertia forces, this is kinematically related to rotation of eccentric shaft and transfer of resultant inertia forces to eccentric journal of the eccentric shaft, at that at change of direction of the vector of the resultant inertia forces to opposite direction in the reference system of the frame, the frame is displaced in the reference system of the bearings of the eccentric shaft in such a way that the direction of projection of the vector of velocity of motion of eccentric journal of eccentric shaft to the line of action of the vector of resultant inertia forces all the time coincides with the direction of the vector of resultant inertia forces, and at t converting to driving forces (traction) at rotation of eccentric shaft the line of effect of resultant inertia forces is rotated with respect to the axis of rotation of the eccentric shaft, with rotation of the line of effect of inertia forces that is kinematically related to rotation of the eccentric shaft and transfer to main bearings of the eccentric shaft of resultant inertia forces, at that at change of direction of the vector of resultant forces to opposite one in the reference system of the frame, the frame with its reference system is as well turned in the reference system of the bearings of the main journals of the eccentric shaft with change of direction of projection to the axis of symmetry of hodograph of the vector of resultant inertia forces related to the reference system of the frame in such way that direction of projection of the vector of resultant inertia forces to the line of symmetry of hodograph is all the time directed to one side.