Relation between angular and linear velocity

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SUMMARY

The discussion clarifies the relationship between angular velocity (ω) and linear velocity (v) in circular motion, specifically defining v as the tangential linear speed. It establishes that when an object is in constant circular motion, there is no radial velocity due to the absence of radial displacement. The centripetal acceleration is attributed to the tangential linear speed, which is evident when an object moves in a circular path. The equation v = rω is derived from geometric principles relating circular arc length to angular displacement.

PREREQUISITES
  • Understanding of circular motion concepts
  • Familiarity with angular velocity and linear velocity
  • Basic knowledge of geometry related to circles
  • Concept of centripetal acceleration
NEXT STEPS
  • Study the derivation of the equation v = rω in detail
  • Learn about centripetal acceleration and its mathematical formulation
  • Explore the differences between tangential and radial velocities
  • Investigate the effects of changing radius on linear and angular velocities
USEFUL FOR

Physics students, educators, and anyone interested in understanding the dynamics of circular motion and the mathematical relationships between angular and linear velocities.

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v=rω.here , what does v(linear velocity) refer to?tangential velocity or radial velocity.further which velocity is responsible for centripetal acceleration?
 
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In this case, v is the tangential linear speed. If you were to cut the string that pulls a ball into a circular path, the string would fly off in a straight line at speed v in the direction tangent to the point on the circle where it was when the string is cut (neglecting relativistic effects). For an object in constant circular motion, there is no linear radial velocity. If an object is spiraling in (for instance, you are shortening the string) then it has both a tangential linear velocity and a radial linear velocity.

The angular speed ω is essentially the angular rotation frequency, i.e. the number of times it goes around in a circle per unit time. You can derive and understand the equation you wrote by first convincing yourself using geometry that the length of a circular arc s is just the angle θ it subtends times its radius r:

s = rθ

If you assume constant r and differentiate both sides with respect to time, you end up with your equation relating linear and angular speeds.
 
Thanks c. Baird . i just got it that there can be no radial velocity as there is no radial displacement.
 

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