Explanation:

Coriolis component acceleration is a fictitious force that arises whenever a point moves along a path that has rotational motion. It is named after the French mathematician Gaspard-Gustave de Coriolis who first described it in 1835. This force is an apparent force that is experienced by a moving object in a rotating reference frame, which is not actually present in the object's actual reference frame.

The Coriolis component acceleration is a result of the combination of two types of motion: linear motion and rotational motion. When an object moves along a path that has a rotational motion, its linear velocity and angular velocity are not in the same direction. This leads to the Coriolis component acceleration, which is perpendicular to both the linear velocity and the angular velocity.

The Coriolis component acceleration is always present whenever an object moves along a path that has rotational motion. This can occur in a variety of situations, including:

- Planetary motion: The Coriolis component acceleration is responsible for the deflection of winds and ocean currents on Earth and other planets.
- Rotating machinery: The Coriolis component acceleration can affect the performance of rotating machinery, such as turbines and centrifuges.
- Projectile motion: The Coriolis component acceleration can affect the trajectory of projectiles, such as bullets and missiles.

In summary, the Coriolis component acceleration is a fictitious force that arises whenever an object moves along a path that has rotational motion. It is perpendicular to the linear velocity and the angular velocity of the object and can have significant effects on the object's trajectory and performance.

The total acceleration of a point with respect to another point in a rigid link is the vector sum of its normal (radial) and tangential components. This holds true when two bodies are in rolling contact, the point in one body that contacts the other body is instantaneously at rest relative to that body.