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Dynamics Introduction
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Kinetics of curvilinear translation
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When a particle moves along a curved
path
which is known, the
equation of motion for the particle may be written in the
tangential
,
normal
, and
binormal
directions.
So if š¯‘‡ acts in the direction of
motion, the particleā€™s speed will
increase
, whereas if it acts in
the opposite direction, the particle will
slow down
In Centripetal force ,Ā It is caused by N which always acts int he
positive
N direction, i.e., toward the pathā€™s Ā
center
of
Ā
curvature
, .
These inertia forces are known as the
centrifugal
inertia
force
or
simply
centrifugal
force
(or reversed normal
effective
force) and the
tangential inertia force
(or reversed tangential
effective force).
A
pendulum
is a weight suspended from a pivot point that is free to swing back and forth under the influence Ā of gravity
Because the string generates a cone while in motion, the Ā system is called a
conical pendulum
Dynamic equilibrium is created by applying the
centrifugal force
acting radially
outward
from the center of the path
The tension š¯‘‡ is also obtained from the
force
Ā polygon
.