What forces must be considered in non-inertial rotating reference frames?

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SUMMARY

This discussion focuses on the dynamics of non-inertial rotating reference frames, emphasizing the necessity of considering real forces such as centripetal force and the role of fictitious forces like centrifugal force. It clarifies that while objects appear at rest in a rotating frame, real forces, including friction, must be accounted for to apply Newton's laws correctly. The centripetal force is defined as the net force acting toward the center, not a distinct type of force. The example of a block on a spinning turntable illustrates how friction acts as the centripetal force while also necessitating the inclusion of centrifugal force in a rotating frame.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with concepts of centripetal and centrifugal forces
  • Knowledge of inertial vs. non-inertial reference frames
  • Basic principles of rotational dynamics
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  • Study the mathematical formulation of centripetal acceleration in rotating systems
  • Explore the implications of fictitious forces in non-inertial frames
  • Investigate applications of rotating reference frames in engineering and physics
  • Learn about the effects of friction in rotational motion scenarios
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Physics students, engineers, and anyone interested in the principles of rotational dynamics and non-inertial reference frames.

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dealing with non-inertial rotating reference frames, real forces such as the centripetal force need to be taken into account,or only the forces that can be really observed within the frame?

because from the perspective of the rotating frame, objects should be at rest. it only appears logical to replace the centripetal force with the centrifugal force when dealing in rotating frames.
 
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Real forces always count. "Real" forces have agents as opposed to "fictitious" inertial forces that are artifacts of using a noninertial frame of reference.

Note: "centripetal" force just means a force that acts toward the center (or the net force acting toward the center)--it's not a separate kind of force.

Example: Imagine a spinning turntable on which a small block sits. The block spins along with the turntable. From an inertial frame, the block is centripetally accelerated; the centripetal force is the friction between turntable and block.

From the rotating frame that very real friction force still acts, but now the acceleration is zero: In addition to the real friction force, one needs to add the "fictitious" centrifugal force in order to use Newton's laws.
 

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