Forces Acting on A Bearing of an Electric Motor for
The Railway Carriage Rounding A Curve
Volume 1 - Issue 1
Ryspek Usubamatov*
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- Kyrgyz State Technical University, Kyrgyzstan
*Corresponding author:
Ryspek Usubamatov, Kyrgyz State Technical University, 720044 Bishkek, Kyrgyzstan
Received: September 10, 2018; Published: September 20, 2018
DOI: 10.32474/ARME.2018.01.000104
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Abstract
Recent investigations in gyroscope effects have demonstrated that their origin has more complex nature that represented in
known publications. On a gyroscope are acting simultaneously and interdependently eight inertial torques around two axes. These
torques are generated by the centrifugal, common inertial and Coriolis forces as well as the change in the angular momentum of
the masses of the spinning rotor. The action of these forces manifests the inertial resistance and precession torques on any rotating
objects. New mathematical models for the inertial torques acting on the spinning rotor demonstrate fundamentally different
approaches for solving of gyroscope problems in engineering. This is the very important result because the stubborn tendency in
engineering is expressed by the increasing of a velocity of rotating objects. The numerous designs of the movable machines and
mechanisms contain spinning components like turbines, rotors, discs and others lead to the proportional increase of the magnitudes
of inertial forces that are forming their processes of work. This work considers the inertial torques acting on the on a rotor of an
electric railway carriage rounding a curve, which expresses the gyroscopic effects.
Keywords: Gyroscope theory; Inertial torques; Spinning rotor
Nomenclature
i. m - Mass of the rotor
ii. g - Gravity acceleration
iii. I - Index for axis ox or oy
iv. J - Mass moment of inertia of the rotor
v. L - Radius of rolling the carriage along the curvilinear path
vi. R - Radius of the rotor
vii. Tam.i, Tcti, Tcr.i, Tin.i - Torque generated by the change in the angular momentum, centrifugal, Coriolis and common inertial
forces respectively, and acting around axis i
vii. Tr.i, Tpi - Resistance and precession torque respectively acting around axis i
ix. ω - Angular velocity of the rotor
x. ωi - Angular velocity of precession around axis i
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