Notes
.
CHAPTER 5: Circular Motion; Gravitation
Uniform Circular Motion Kinematics
Uniform circular motion describes the movement of an object in a circular
path at constant speed.
The velocity vector, however, is constantly changing in
order for the object to stay on the circular path.
At any point in the path, the velocity vector is tangent to the circular
path in the direction of motion.
The acceleration at any point is directed toward the center of the circle.
This radial acceleration is given by ar = v2/r
At any point, the velocity and radial acceleration vectors are perpendicular
The number of revolutions per second, the frequency f, is given in seconds.
The period T is the reciprocal of the frequency, and is the time in seconds
for each revolution.
From the above, it can be seen that the
speed is given
by 2pr/T
Uniform
Circular Motion Dynamics
åFR
= mv2/r
This force, directed toward the circle’s center, is that required to keep
the object in
circular motion
Remove the force, and the object continues in the direction of the velocity
vector at that point.
For cars, road friction provides the inward force to move in a circle.
Satellites use gravity to provide the force for
circular orbits
Non
Uniform Circular Motion
This is the situation when for net force on an object is not directed toward
the center of the circle.
In this case, the force vector can be broken into 2
perpendicular components
]
Inward directed radial force: FR
]
Tangential force: FTan
The acceleration can also be broken into two components
]
Inward radial acceleration: aR
]
Tangential acceleration: aTan
Note the speed is changing in this case, as a result of
the tangential force resulting in a tangential acceleration
The magnitude of the acceleration at any point can be
found from the Pythagorean theorem, using
Newton’s
Law of Universal Acceleration
The magnitude of the attractive force between two
objects is given by
F = Gm1m2/r2
Where G is a proportionality constant, m1 is the mass of one object, and m2 is the mass of the other object, and r is the distance between the
centers of the
two objects.
The value for G was first determined experimentally by
Cavendish, about 100 years after Newton