Every time an object moves along a non-linear trajectory, we are sure some force acts on the object. This happens even if the speed of the object is constant: the object must experiences some forces because its direction of motion changes!
Every time an object describes a curved trajectory it undergoes an acceleration. In effect along the curve its direction of motion changes, that means a change in velocity, that means an acceleration.
What are direction and magnitude of this acceleration? We will try to answer the question in the simple case of uniform circular motion.
An object describing a circumference with a constant speed represents this kind of motion.
For such an object the direction of the velocity vector continually changes, so the object continually experiences an acceleration.
since the definition of instantaneous acceleration is
the direction of is the same of change in velocity vector .
The direction of the can be computed as follows:
We chose a very short time interval between two positions.
We compute the difference between the velocities and at those positions (see the figure below).
The direction of the acceleration . is equal to the direction of the change in velocity .
(best draws are available on page 76 in the textbook).
Following this line of reasoning we conclude that the acceleration is always directed toward the centre of the circle and for this reason we call this acceleration CENTRIPETAL ACCELERATION .
The centripetal acceleration has
Therefore the magnitude of the centripetal acceleration has a double and direct dependence on speed and an inverse dependence on the radius. Using maths:
.
According to the Newton’s Second Law, if an mass object covers a curved trajectory, a centripetal force
is acting.
where is the speed of the object, and is the bend radius of the covered curve.