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This can be achieved by the installation of an elastic corrector with negative rigidity. A negative rigidity in the force push-spring lever with balance corrector (FC-Ipu) is based on the lever 1 profile that reduces arm a of the force pushing down spindle 2 at its higher position even if the force in the spring 3 increases. Balancing body 4 on the lever compensates for the changes in the spindle force due to a different orientation of the structure in the gravity field. A negative rigidity in the force pull- spring lever corrector (FC-IpI) is based on the increase of arm a of spring 1's action on lever 2 at the higher'posi& of spindle 4.
General Problems of Precision Kinematics It is known that at each instant, the motion of any rigid body can be thought of as the superposition of both a translational and rotational motion. The motion of the rigid body is a combination of the translational motion with a linear speed V and the rotational motion with angular speed R, which in a given instant corresponds to the certain origin 0 in Fig. 1-4a. Both translational and rotational velocities are the vector quantities. Hence in this case, we have bivector (motor) of two superposed vectors, V and R.
As a result, the acting on the spindle force changes accordingly, compensating for the influence of gravity. IC-I, 11. The influence-damper corrector (IC-I) can be used as a liquid or air damper in the vibration field or in the dynamic motion of the elastic structure's elements. The influence-speed retraction's corrector (IC-11) is useful when the speed of spindle 1's motion released after its retraction should be stable. In this case, the 20 I. PROBLEMS AND METHODS speed of spindle 1's motion after its release by pushing stop 2 is practically independent from the speed of stop 2's displacement.