Why is the force of the spring equal to the centripetal force?

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SUMMARY

The discussion clarifies the relationship between the force of a spring and centripetal force in a circular motion scenario. Specifically, when a mass is attached to a spring or string and rotates around a fixed point with a radius of 4 meters, the net radial force exerted by the spring equals the centripetal force required to maintain circular motion. This is established through Newton's third law, where the tension in the string or spring provides the necessary centripetal force, which is not a distinct force but rather a resultant force that acts inward. The centripetal acceleration is defined as ar = v2/r, linking the tension directly to the mass and acceleration.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with centripetal acceleration and its formula
  • Knowledge of spring force represented by F = kx
  • Basic concepts of circular motion dynamics
NEXT STEPS
  • Study the derivation of centripetal acceleration and its implications in circular motion
  • Explore the relationship between tension in strings and centripetal force in rotating systems
  • Investigate potential energy calculations in spring systems
  • Learn about the differences between real forces and fictitious forces in physics
USEFUL FOR

Physics students, educators, and anyone interested in understanding the dynamics of circular motion and the interplay between spring forces and centripetal forces.

Perseverence
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Homework Statement


A string is rotated around a point with a radius of 4 meters. Calculate the potential energy stored in the spring

Homework Equations


F = KX

The Attempt at a Solution


The solution to the problem involves making the force of a spring equal to the centripetal force. I don't really understand why that would be. Both forces Point towards the center of the circle. How do we know that they are equal? They are not counterbalancing each other if they are both going in the same direction.
 
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But you know that's not the case by experiment as the string stretches and the object moves around in a circular path. Hence while the centripetal force is directed inward, you must look more carefully at the direction of the string tensile force.

http://en.citizendium.org/wiki/Centripetal_force

The figure shows the radially inward centripetal force FC provided by the string that is necessary to force the object to travel the circular path of radius R at a constant speed v. (The "speed" of the body is the magnitude of its velocity, without regard to direction.) The body in turn provides an equal but oppositely directed tensile force FT on the string as shown to the left (a consequence of Newton's law that to every force there is an equal and opposite reaction force), and the string also is subject to the same tensile force at its other end, in opposite direction, as provided by the fixed centerpost.
 
It's a common confusion regarding the centripetal force.
It's not a real force - it's just a value some other force has to have in order to make a mass go around in circles.
So, if you have a mass on a string (or spring) going in circles, then you know that the net radial force is precisely equal to the centripetal force.
 
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Perseverence said:

Homework Statement


A spring is rotated around a point with a radius of 4 meters. Calculate the potential energy stored in the spring.
Just to check you have the right picture in mind: how long is the rotating spring ?
 
Bandersnatch said:
It's a common confusion regarding the centripetal force.
It's not a real force - it's just a value some other force has to have in order to make a mass go around in circles.
So, if you have a mass on a string (or spring) going in circles, then you know that the net radial force is precisely equal to the centripetal force.

Some other force or forces. Sometimes several forces combine to provide the centripetal force needed to make the mass move in a circle.
 
Bandersnatch said:
It's a common confusion regarding the centripetal force.
It's not a real force - it's just a value some other force has to have in order to make a mass go around in circles.
It's probably better to say the centripetal force is not yet another force; rather, it's a resultant force that points radially inward. I wouldn't say it's not a real force, as that might cause confusion with the concept of a fictitious force, like the centrifugal force.

I usually avoid the idea of a centripetal force altogether. When an object follows a circular path, it experiences a centripetal acceleration, ##a_r = \frac{v^2}{r}.## It shows up on the ##ma## side of the second law, not on the ##\sum F## side.
 
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vela said:
I usually avoid the idea of a centripetal force altogether. When an object follows a circular path, it experiences a centripetal acceleration, ##a_r = \frac{v^2}{r}.## It shows up on the ##ma## side of the second law, not on the ##\sum F## side.
I like that. So the tension in the string/rope/etc. is equal to the mass times the centripetal acceleration.
 
I mostly agree with @vela in that "centripetal" is an adjective that indicates the direction of a force relative to some coordinate system, but I wouldn't necessarily call it the resultant. "Centripetal" is used the same way as the adjectives "normal", "horizontal", vertical", etc. to label the direction of forces. For example, the Earth exerts a vertical force on a book that is at rest on a table top; the Earth exerts a centripetal force on the book when it is in a circular orbit around the Earth. Same Earth, same book, same interaction between the two but different reference frames.
 

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