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Rotational motion
Rotational motion
• We have learned about
  translational motion up to this
  point…
• Now, we will venture into
  ROTATIONAL MOTION of a rigid
  body
    – Rigid body: a body with a
      definite shape that does not
      change
• Rigid bodies can be analyzed as:
    – The translational motion of its
      center of mass and the rotational
      motion about its center of mass.
• We will concentrate on purely
  rotational motion – all points in
  the body move in circles.
Rotational Motion
                                                  C
Last chapter, we talked about an                          B
object in uniform circular motion:
• Period
• Tangential velocity                 D
                                              r
• Centripetal Acceleration                m
                                                      v
• Centripetal force                               A
Now, we will talk about an object’s
motion as it revolves in a
circle, when it is uniform or non-
uniform!
Rotational Motion
• Now we will describe the circular motion of an
  object using angles, in terms of its:
  – Angular displacement θ [radians]
  – Angular velocity ω [rad/sec, rev/sec]
  – Angular acceleration α[rad/sec2]
Angular Displacement
          • Angular Displacement (θ)
            is the angle that a rotating
            object goes through.
          • We measure this in radians
             – A fraction of a revolution can
               be measured in
               degrees, grads or radians
          • A degree is 1/360 of a
            revolution
          • We can convert to radians
            using:
             – π radians = 180 degrees
             – One revolution = 2 radians
             …and use factor label method!
Example: Angular Displacement
• A rubber stopper is twirled over a student’s head in a
  physics lab. Calculate the angular displacement of
  the stopper if it travels:
   –   30 degrees
   –   0.25 revolutions
   –   90 degrees
   –   1700 degrees
   –   12 revolutions
Angular distance θ in radians
      We can convert from linear distance
      (meters) to angular distance (radians) by:
      • first converting to radians
      • Use equation
                         θ=s
                             r
                        s = arch length in meters (distance)
                        r = radius of circular path (meters)
                        θ = angle in radians
Example: finding arc length
• What is the angular displacement of a rubber
  stopper that is twirled over a physics teacher’s head
  at a radius of 0.4 m and it travels 3.0 meters?
Example: arc length
Example 8-1 from book: A particular bird’s eye can distinguish
objects that subtend an angle no smaller than about 3x10-4 rad.
How small of an object can the bird just distinguish when flying
at a height of 100 m?
Subtend: The angle formed by an object at a given external point




                                    3 cm
Angular velocity ω
         In rotational motion, we usually describe
         the angular velocity as revolutions per
         second (rev/sec, rps), or radians per
         second
         • You will often have to convert this
             number, since it is usually given as a
             frequency (revolutions per time frame)
         • Conversion from linear velocity:

              ω= v
                  r
             v = tangential (linear) velocity (m/s)
             r = radius of circular path (meters)
             ω = angular velocity (rad/sec)
Angular Velocity


   Unlike tangential
 velocity, the angular
velocity is the same at
every point on a rigid
  body, like a wheel
Example: angular velocity
Example 8-3: What is the angular and linear speed of a child
sitting 1.2 m from the center of a steadily rotating merry-go-
round that makes one complete revolution in 4.0 seconds?
Angular acceleration α
                 Angular acceleration occurs when the
                 angular velocity changes over time.
                 • It acts in the direction of rotation in a
                   circular motion (NOT the same as
                   centripetal acceleration)
                 • In this case, we must also introduce
                   tangential acceleration (at) since the
                   tangential velocity is changing
                       – If there is angular acceleration, there will
                         also be tangential acceleration
                 • We can use the following conversion:
    α= at
        r                                      ar= ω2r
   a = tangential (linear) acceleration (m/s) ar = radial (linear) acceleration (m/s)
   r = radius of circular path (meters)       r = radius of circular path (meters)
                                      2)
   ω = angular acceleration (rad/sec          ω = angular acceleration (rad/sec2)
Example: Angular Acceleration
What is the tangential and angular acceleration of a child seated
1.2 m from the center of a steadily rotating merry-go-round that
makes one complete revolution in 4.0s?
Linear & rotational motion equivalents
Now let’s re-write the linear motion equations using our rotational motion values!
Examples: kinematic equations
Ex 8-5: A centrifuge rotor is accelerated from rest to 20,000 rpm
in 5.0 min. What is its average angular acceleration?
Examples: kinematic equations
Ex 8-5: A centrifuge rotor is accelerated from rest to 20,000 rpm in
5.0 min. (a) What is its average angular acceleration? (b) through
how many revolutions has the centrifuge rotor turned during its
acceleration period? Assume constant angular acceleration.




                                             a. 7.0 rad/s2
                                             b. 50,000 revs
Rotational motion pt2

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Rotational motion pt2

  • 2. Rotational motion • We have learned about translational motion up to this point… • Now, we will venture into ROTATIONAL MOTION of a rigid body – Rigid body: a body with a definite shape that does not change • Rigid bodies can be analyzed as: – The translational motion of its center of mass and the rotational motion about its center of mass. • We will concentrate on purely rotational motion – all points in the body move in circles.
  • 3. Rotational Motion C Last chapter, we talked about an B object in uniform circular motion: • Period • Tangential velocity D r • Centripetal Acceleration m v • Centripetal force A Now, we will talk about an object’s motion as it revolves in a circle, when it is uniform or non- uniform!
  • 4. Rotational Motion • Now we will describe the circular motion of an object using angles, in terms of its: – Angular displacement θ [radians] – Angular velocity ω [rad/sec, rev/sec] – Angular acceleration α[rad/sec2]
  • 5. Angular Displacement • Angular Displacement (θ) is the angle that a rotating object goes through. • We measure this in radians – A fraction of a revolution can be measured in degrees, grads or radians • A degree is 1/360 of a revolution • We can convert to radians using: – π radians = 180 degrees – One revolution = 2 radians …and use factor label method!
  • 6. Example: Angular Displacement • A rubber stopper is twirled over a student’s head in a physics lab. Calculate the angular displacement of the stopper if it travels: – 30 degrees – 0.25 revolutions – 90 degrees – 1700 degrees – 12 revolutions
  • 7. Angular distance θ in radians We can convert from linear distance (meters) to angular distance (radians) by: • first converting to radians • Use equation θ=s r s = arch length in meters (distance) r = radius of circular path (meters) θ = angle in radians
  • 8. Example: finding arc length • What is the angular displacement of a rubber stopper that is twirled over a physics teacher’s head at a radius of 0.4 m and it travels 3.0 meters?
  • 9. Example: arc length Example 8-1 from book: A particular bird’s eye can distinguish objects that subtend an angle no smaller than about 3x10-4 rad. How small of an object can the bird just distinguish when flying at a height of 100 m? Subtend: The angle formed by an object at a given external point 3 cm
  • 10. Angular velocity ω In rotational motion, we usually describe the angular velocity as revolutions per second (rev/sec, rps), or radians per second • You will often have to convert this number, since it is usually given as a frequency (revolutions per time frame) • Conversion from linear velocity: ω= v r v = tangential (linear) velocity (m/s) r = radius of circular path (meters) ω = angular velocity (rad/sec)
  • 11. Angular Velocity Unlike tangential velocity, the angular velocity is the same at every point on a rigid body, like a wheel
  • 12. Example: angular velocity Example 8-3: What is the angular and linear speed of a child sitting 1.2 m from the center of a steadily rotating merry-go- round that makes one complete revolution in 4.0 seconds?
  • 13. Angular acceleration α Angular acceleration occurs when the angular velocity changes over time. • It acts in the direction of rotation in a circular motion (NOT the same as centripetal acceleration) • In this case, we must also introduce tangential acceleration (at) since the tangential velocity is changing – If there is angular acceleration, there will also be tangential acceleration • We can use the following conversion: α= at r ar= ω2r a = tangential (linear) acceleration (m/s) ar = radial (linear) acceleration (m/s) r = radius of circular path (meters) r = radius of circular path (meters) 2) ω = angular acceleration (rad/sec ω = angular acceleration (rad/sec2)
  • 14. Example: Angular Acceleration What is the tangential and angular acceleration of a child seated 1.2 m from the center of a steadily rotating merry-go-round that makes one complete revolution in 4.0s?
  • 15. Linear & rotational motion equivalents Now let’s re-write the linear motion equations using our rotational motion values!
  • 16. Examples: kinematic equations Ex 8-5: A centrifuge rotor is accelerated from rest to 20,000 rpm in 5.0 min. What is its average angular acceleration?
  • 17. Examples: kinematic equations Ex 8-5: A centrifuge rotor is accelerated from rest to 20,000 rpm in 5.0 min. (a) What is its average angular acceleration? (b) through how many revolutions has the centrifuge rotor turned during its acceleration period? Assume constant angular acceleration. a. 7.0 rad/s2 b. 50,000 revs