In physics, we say that a body has acceleration when there is a change in the velocity vector, either in magnitude or direction. In previous sections, we have seen that acceleration can be broken down according to the effect that it produces in the velocity, in the following manner:

• tangential acceleration. Responsible for the change in the magnitude of the velocity vector
• normal or centripetal acceleration. Responsible for the change in the direction of the velocity vector

Both concepts are known as the intrinsic components of acceleration and their values can be used to classify motion, as we will see below.

• Motion in which normal acceleration is equal to 0 is rectilinear motion and it will be accelerated rectilinear motion or rectilinear uniform motion depending on its tangential acceleration.
• Motion in which the normal acceleration is different than 0 is considered to be curvilinear or circular depending on whether the radius of curvature $\rho$ remains constant. Motion with a constant radius of curvature have a circumference as trajectory and they will be accelerated or not based on the value of the tangential acceleration ${\stackrel{\to }{a}}_{t}$

In the following table, you can find a classification of motion according to the values of the intrinsic components of the acceleration (normal and tangential acceleration).

CLASSIFICATION OF MOTION ACCORDING TO THE INTRINSIC COMPONENTS OF THE ACCELERATION

Intrinsic components of the acceleration at
${a}_{t}=0$ ${a}_{t}=\text{cte}\ne 0$ ${a}_{t}\ne \text{cte}$
an ${a}_{n}=0$
rectilinear
Uniform rectilinear motion (u.r.m.) Uniformly accelerated rectilinear motion (u.a.r.m.) Accelerated rectilinear motion
${a}_{n}>0$
$\rho =R=\text{cte}$
circular
Uniform circular motion (u.c.m.) Uniformly accelerated circular motion (u.a.c.m.) Accelerated circular motion
${a}_{n}>0$
$\rho \ne \text{cte}$
Non-circular curvilinear motion