Centripetal acceleration and tangential acceleration

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SUMMARY

The discussion centers on the relationship between centripetal acceleration and tangential acceleration in circular motion. Tangential acceleration (aT) is defined as aT = r * α, where α represents angular acceleration, which is calculated as α = (ωf - ω0) / (tf - t0). In contrast, centripetal acceleration (aC) is expressed as aC = r * ωf², indicating its dependence solely on the final angular velocity (ωf) rather than the initial angular velocity (ω0). The physical explanation provided emphasizes that centripetal acceleration is necessary to maintain circular motion, directing the mass toward the center of the circular path.

PREREQUISITES
  • Understanding of circular motion dynamics
  • Familiarity with angular velocity and acceleration concepts
  • Knowledge of the equations for tangential and centripetal acceleration
  • Basic physics principles regarding forces and motion
NEXT STEPS
  • Study the derivation of angular acceleration in circular motion
  • Explore the implications of varying angular velocities on centripetal acceleration
  • Investigate the effects of different radii on centripetal acceleration
  • Learn about the applications of centripetal acceleration in real-world scenarios, such as in roller coasters or planetary motion
USEFUL FOR

Students of physics, educators teaching circular motion concepts, and engineers involved in mechanical design requiring an understanding of acceleration in circular paths.

Maxo
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When having a circular acceleration motion, we have both tangential acceleration and centripetal acceleration.

The tangential acceleration is aT=r*α where α=1/2*(ωf0). So we can see tha aT is dependent on both the initial angular velocity ω0 and the final ωf).

For centripetal acceleration, we instead have aC=r*ωf2.

My question is, how come the centripetal acceleration is only dependent on the final angular velocity, and not the initial?
Is there a physical explanation for this?
 
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First: α isn't 1/2*(ωf0). The correct equation is α = (ωf0)/(tf-t0).

Second: The equation above is the expression for the AVERAGE angular acceleration. If the circular motion is UNIFORMLY accelerated than you can use the average angular acceleration to calculate the tangential speed since angular acceleration is constant, otherwise you have to use the instantaneous angular acceleration - say αf and the expression for tangetial acceleration becomes aTf = r αf
 
Ok thanks for the correction. But I still wonder why the centripetal acceleration is only dependent on the final angular velocity, and not the initial angular velocity. Is there a physical explanation for this?
 
centripetal acceleration is caused to continue circular motion so at every point. so at that point it has to accelerate the mass toward center so as to change it direction.
now for at the point it has angular velocity omega then centripetal acceleration will vary with that only
 

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