Uniform circular motion is motion along a circular path with constant speed. The word "uniform" does not mean everything stays the same. The speed stays the same, while the direction of motion keeps changing because the object follows a curved path.
Picture a small car moving around a round track. Every second, the car can cover the same length of track. But the car's velocity on the right side of the track points in a different direction from its velocity at the top of the track.
In uniform circular motion, speed is constant, but velocity still changes because its direction changes.
That is the key difference between speed and velocity. Speed only describes how fast the object moves along the path. Velocity describes both speed and direction.
Car on a Circular Track
Change the period to see the car complete each lap at a different speed.
In straight-line motion, position is often read as distance from zero. In circular motion, position is easier to read with an angle. The angle swept by the object is called angular displacement.
If an object moves from a reference line and sweeps an angle Δθ in time Δt, its angular velocity is:
ω=ΔtΔθ
The symbol ω is called omega. Its unit is radians per second, written rad/s. Radians are used because one full turn equals 2π radians.
One full revolution can be read in two ways. Period, written T, is the time needed for one revolution. Frequency, written f, is the number of revolutions each second.
They are reciprocals:
f=T1
ω=T2π=2πf
When the period is smaller, the object completes a revolution faster. As a result, its frequency and angular velocity are larger.
At every point on a circular path, velocity points tangent to the circle. Centripetal acceleration points toward the center. These two directions are perpendicular, so an object can have constant speed and still have acceleration.
Imagine a small object on the right side of the circle moving counterclockwise. Its velocity points upward along the path, while its acceleration points left toward the center. This direction pair is what makes circular motion different from ordinary straight-line motion.
Linear velocity is the object's speed along the circular path. If the radius is r, one full circumference is 2πr. Because one revolution takes time T, the linear velocity is:
v=T2πr
v=ωr
The formula v=ωr means two objects with the same angular velocity do not always have the same linear velocity. The object farther from the center travels a longer path, so its linear velocity is larger.
Even though speed is constant, the velocity direction keeps turning. Changing the direction of velocity requires acceleration. In uniform circular motion, this acceleration is called centripetal acceleration.
as=rv2
as=ω2r
Centripetal acceleration always points toward the center of the circle. So do not think of this acceleration as pointing along the object's motion. Velocity is tangent to the path, while centripetal acceleration points inward.
Suppose a small car moves on a track with radius 4 m and completes one revolution in 6 s.
Its angular velocity is:
ω=T2π=62π=3π rad/s
Its linear velocity is:
v=ωr=3π(4)=34π m/s≈4.19 m/s
Its centripetal acceleration is:
as=rv2=4(4.19)2≈4.39 m/s2
So the car moves with constant speed of about 4.19 m/s, but it still has acceleration of about 4.39 m/s2 because the direction of its velocity keeps changing.
