Centripetal force is not a fundamental force itself, but rather a net force acting on an object that causes it to accelerate towards the center of its circular path. Without this inward pull, the object would continue in a straight line due to inertia.
The magnitude of centripetal force ($F_c$) is calculated using the formula: $F_c = rac{mv^2}{r}$, where m is the mass of the object, v is its velocity, and r is the radius of the circular path. This shows that a higher velocity or a smaller radius requires a larger centripetal force.
Centripetal force is observed in many everyday phenomena and scientific applications:
A common misconception is the existence of a ‘centrifugal force’ pushing outwards. In reality, what’s perceived as centrifugal force is simply the object’s inertia resisting the change in direction caused by the centripetal force.
Q: What happens if centripetal force disappears?
A: The object will move in a straight line tangent to its path at the moment the force is removed.
Q: Is centripetal force always constant?
A: Its magnitude can vary if the speed or radius of the circular path changes.
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