Username:
   
Password:

I forgot my username or password.

In support of all the students who are displaced from school due to the Corona virus. Access to physics zone and chemistry zone lessons are now available free of charge. This will be maintained at least through August 1st 2020. Learn and be well.

Physics Lessons Review Links Solutions Physics Shop

Centripetal Force - The Real Force

Whenever an object moves in a circular path the object is accelerating because the velocity is constantly changing direction.  All accelerations are caused by a net force acting on an object.  In the case of an object moving in a circular path, the net force is a special force called the centripetal force (not centrifugal!).   Centripetal is Latin for "center seeking".  So a centripetal force is a center seeking force which means that the force is always directed toward the center of the circle.  Without this force, an object will simply continue moving in straight line motion.

Imagine swinging a rope with a mass attached to the end, around in a circle above your head:
Compare each of the following animations to the original one in the top left.  Look carefully for what has changed in each one.

large mass swinging on a rope small mass swinging on a rope
  • The force of tension from the rope, shown as FT, is what provides the required centripetal force needed to keep the ball in the circular path.
  • The smaller the mass, the smaller the centripetal force you will have to apply to the rope.  Smaller masses require smaller centripetal force.
mass swinging on a rope with small velocity

mass swinging on a rope with large velocity
  • The smaller the velocity of the object, the less centripetal force you will have to apply.
  • The smaller the length of rope (radius), the more centripetal force you will have to apply to the rope.
  • Notice that the centripetal force (FT)  and the centripetal acceleration (A) are always pointing in the same direction. (the force causes the acceleration)
Cut the rope. (13k)
  • If you let go of the rope (or the rope breaks) the object will no longer be kept in that circular path and it will be free to continue on with its current velocity.  
  • It goes off on a tangent!

The formula for centripetal force is centripetal force formula F = m v squared over r  where m represents the mass of the object, v is the speed (magnitude of the velocity) and r is the radius from the center of the circle to the object.  A centripetal force ends up being a net force and a net force always causes an acceleration in the direction of the net force.  So if the force is center seeking (centripetal) then the acceleration is also centripetal.  The formula for centripetal acceleration is  centripetal acceleration formula a = v squared over r.    [Notice that if you multiply this by mass (m) you get the formula for centripetal force...that's because a net force is equal to mass times acceleration.]

It is conceptually better to think about the Centripetal force that is calculated from the formula as a requirement.  If you satisfy the requirement, then you have circular motion at the radius and speed used in the formula.  If you do not satisfy the requirement, then the object moves into a larger curve (which requires less force) or defaults into straight line motion (going off on a Tangent).

Enough Fc In this animation, the "sticky" or adhesive force from the mud to the tire tread is large enough to be the centripetal force required to keep the mud in a circular path as the tire spins.
Not enough Fc In this animation, the tire is spinning faster which means a larger centripetal force is required to keep the mud in the circular path of the tire.  The adhesive force of the mud to the tire is not large enough to meet the requirement.   The mud begins to move into a larger circular path but as soon as it is not touching the tread there is no force (other than gravity) and so the mud continues with the velocity it had at the instant it was no longer touching the tread.  .  It followed Newton's first law!
NEXT: Centrifugal force