Use of a non-inertial reference frame in a problem involving rotation?

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SUMMARY

The discussion focuses on analyzing the radial acceleration of a block sliding on a rotating disk with angular velocity ω. The user proposes using "centrifugal force" to calculate the forces acting on two blocks connected by a string. The community confirms that this approach is valid within a non-inertial reference frame, suggesting that the radial acceleration can also be derived using the formula a = ω²r, which aligns with Newton's laws. The conversation emphasizes the importance of distinguishing between fictitious and real forces in rotational dynamics.

PREREQUISITES
  • Understanding of rotational dynamics and angular velocity (ω).
  • Familiarity with Newton's laws of motion.
  • Knowledge of centripetal and centrifugal forces.
  • Basic principles of tension in strings and forces in a non-inertial reference frame.
NEXT STEPS
  • Study the application of Newton's laws in non-inertial reference frames.
  • Learn about the derivation and implications of the formula a = ω²r in rotational systems.
  • Explore the differences between fictitious forces and real forces in physics.
  • Investigate the dynamics of connected bodies in rotational motion, including tension analysis.
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Students studying physics, particularly those focusing on rotational dynamics, mechanics, and the application of Newton's laws in non-inertial frames.

serllus reuel
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Homework Statement


A disk rotates with angular velocity ω. It has a groove cut along the diameter in which two blocks of mass m and M slide without friction. They are connected by a light string of length l, fixed by a catch with block m a distance r from the center (r + radius of M = l). The catch is then removed.
Find the initial radial acceleration of block m.


My ideal was to imagine a "centrifugal force" acting on each of the blocks. The magnitudes would then be mrω^2 and M(l-r)ω^2, from the formula for centripetal force. Then, I would treat the (rotating) diameter as an x-axis of sorts, thinking of the centrifugal forces as forces on the blocks, and using F=ma and the tension in the string to find the acceleration along the axis, which would turn out to be the radial acceleration.

Is this approach valid? Even if it is, is there an equivalent approach using only real forces? I have tried a few methods, but they generally simplify to the above method. Is there anything I have not thought of?

Finally, I want to note that this came up in the "Newton's laws" chapter of a book, so I really should be using real forces.

Thanks in advance
 
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hi serllus reuel! :smile:

(try using the X2 button just above the Reply box :wink:)
serllus reuel said:
My ideal was to imagine a "centrifugal force" acting on each of the blocks. The magnitudes would then be mrω^2 and M(l-r)ω^2, from the formula for centripetal force. Then, I would treat the (rotating) diameter as an x-axis of sorts, thinking of the centrifugal forces as forces on the blocks, and using F=ma and the tension in the string to find the acceleration along the axis, which would turn out to be the radial acceleration.

Is this approach valid?

yes :smile:

in that frame, the diameter is stationary, so just use F = ma in the usual way
Even if it is, is there an equivalent approach using only real forces?

yes, using a = ω2r :wink:

(in your first method, mω2r is on the LHS of F = ma as part of F; in the second method it's on the RHS, as part of ma)
 
tiny-tim said:
yes, using a = ω2r :wink:

(in your first method, mω2r is on the LHS of F = ma as part of F; in the second method it's on the RHS, as part of ma)


aha, I see.

thanks.
 

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