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A Perturbation Solution of the Equations of Motion of a Gyroscope

Journal of Applied Mechanics, 1959
Abstract A perturbation method of solution is outlined for the nonlinear equations of motion of free and forced vibration of a two-gimbal gyro. Results are given for the term displayed in the solution which indicates that the outer gimbal of the gyro will not oscillate about its initial center position, but will acquire a steady rate of ...
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An exceptional case of motion of the kovalevskaia gyroscope

Journal of Applied Mathematics and Mechanics, 1983
zbMATH Open Web Interface contents unavailable due to conflicting licenses.
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Relativistic gyroscopic motion and aberration

Physical Review D, 1976
A new generally covariant method to calculate the motion of the axis of an orbiting gyroscope, with respect to the direction of fixed stars, is presented. The method includes general-relativistic aberration effects and gives frame-independent results which can be compared directly with the proposed NASA gyroscope experiment.
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Towards an understanding of gyroscopic motion

Physics Education, 1968
Common treatments of gyroscopic motion in textbooks at the student level tend to be difficult to follow physically although trivial mathematically, and sometimes simplify matters to the point of actually giving an incorrect description of the motion of a gyroscope when under the influence of an external torque.
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Conservative Motion of Tops and Gyroscopes

1997
Rigid body motion is of fundamental interest in mathematics, science and engineering. In this chapter we will introduce a simplistic approach to this area of study in the spirit of modern molecular mechanics. We will consider first a discrete tetrahedral body and simulate its motion when it spins like a top whose contact point with the XY plane is ...
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The Motion of a Gyroscope Mounted in Gimbals

2000
Equations of motion of an astatic gyroscope mounted in gimbals in presence of a viscous friction in the gimbals axes have the form [33] $$\left[ {{A_2} + (A + {A_1}){{\cos }^2}\beta + {C_1}} \right]\frac{{{d^2}\alpha }}{{d{T^2}}} + ({C_1} - A - {A_1})\sin (2\beta )\frac{{d\alpha }}{{dT}}\frac{{d\beta }}{{dT}} + H\cos \beta \frac{{d\beta }}{{dT}} + {
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Gyroscopic Perpetual Motion Machine

The construction of a perpetual motion machine has remained an unfulfilled objective in the mechanical and physical sciences community. Despite numerous attempts over the centuries, none has achieved success. At present, such machines are considered impossible as they appear to contradict the principle of energy conservation, a fundamental pillar for ...
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Adaptive scheduling of acceleration and gyroscope for motion artifact cancelation in photoplethysmography

Computer Methods and Programs in Biomedicine, 2022
Antonino Parisi, Luca Faes, Heewon Chung
exaly  

Out-of-plane motion detection in encapsulated electrostatic MEMS gyroscopes: Principal parametric resonance

International Journal of Mechanical Sciences, 2021
Shahrokh Hosseini Hashemi   +2 more
exaly  

On motion of kowalewski's gyroscope

Journal of Applied Mathematics and Mechanics, 1964
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