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Linear & Angular Motion
                       (part 2)


   Objectives:
   • Learn the relationship between linear and
     angular velocity for a body in rotation
   • Learn to compute the tangental and radial
     acceleration of a body in rotation
   • Learn how to analyze general motion
   • Become familiar with methods for measuring
     kinematic quantities




          Linear & Angular Velocity
The instantaneous linear velocity (v) of a point on a
  rotating body is:
• In a direction tangental to the path of motion
• Has a signed magnitude (v) of:
                                            v
      v=rω

 where:                             ω
 • r = radius of rotation                       r
 • ω = angular velocity
   in radian/s !

                         axis of rotation




                                                        1
Finding the Tangental Direction
• Instantaneous linear velocity directed ±90° from the
  line segment from the axis of rotation to the point

          v
                 θ+90°


    ω                                             (θ – 90°)

                                         ω          v
         θ                          θ

    ω counterclockwise              ω clockwise
    (ω and v positive)           (ω and v negative)




              Example Problem #1
  A quarterback starts to throw with his arm angled
    170° with respect to the forward (+x) direction.
  He accelerates his arm forward (clockwise) at
    3000°/s2
  He releases the football when his arm is at 120°
  His arm is 70 cm long.
  What is the linear velocity of his hand at the instant
    he releases the football?




                                                              2
Radial & Tangental Velocity Changes
• The linear velocity of a rotating object changes:
  – along the path of         v2
    motion (tangental)
  – perpendicular to
    the path of motion             ∆vradial        ∆vtangental
    (radial)
                                                     v1
  • Thus, it must also                        v2
    accelerate in the         ω2
    tangental & radial
    directions                               ω1




     Radial & Tangental Acceleration
• The acceleration of a body in angular motion can
  be resolved into two components:
  – Tangental:
    along the path of
    motion                                atangental
  – Radial:
                          a
    perpendicular to
    the path of                          aradial
    motion

   a = atangental + aradial
                                         α
                                     ω




                                                                 3
Tangental Acceleration
• Component of acceleration directed along a tangent
  to the path of motion
• Represents a change in linear speed

            v2 – v1                          v2
   at =
            t2 – t1
                                                                     v1
                                                        at
• If r is constant:
                                                  r2
            r ω2 – r ω1
   at =
              t2 – t1                   ω2
                                                                r1
    at = r α      α in radian/s2 !                 ω1




                  Radial Acceleration
• Component of acceleration directed towards the
  center of curvature
• Represents a change in direction
                                                        v
             v2
     ar =
              r

• If r is constant:                                    ar
          rω      2
                                             ω
     ar =                                                   r
           r
     ar = r ω2        ω in radian/s !




                                                                          4
Tangental & Radial Directions
• Tangental acceleration directed ±90° from the line
  segment from the axis of rotation to the point
• Radial acceleration always directed inward
           at       θ+90°

           ar                      ar            (θ – 90°)
  α
                                                      at
                                        α
           θ                       θ
      α counterclockwise           α clockwise
       (α and a t positive)    (α and a t negative)




          Release of a Rotating Object

• At the instant that               v2 without ar
  radial acceleration
  is removed,
                      v2 with ar
  an object
  becomes
  projected in the                          v1
  tangental direction

                                        r

                                   ω




                                                             5
Example Problem #2
 In problem #1, what is the average acceleration
    of the hand-and-ball along the path of motion
    between the start of the throw and the release
    of the ball?
 At the instant before the football leaves the hand,
    what are its linear velocity and acceleration?
 At the instant after the football leaves the hand,
    what are its linear velocity and acceleration?
 If we know that the ball is released from a height
    of 2.1 m, can we determine how far downfield it
    can travel?




           Example Problem #3
Two runners are racing the 200 m.
Runner #1 is in lane 1, Runner #2 is in lane 8.
The inside radius of the track is 36.8 m. Each lane
   is 1.1 m wide.
If both runners try to run the curve at 9 m/s, how
   much will each runner need to accelerate in the
   radial direction?




                                                       6
Relative Linear Velocity
• Apparent velocity of a 2 nd point to an observer at
  a 1st moving point
• Compute absolute velocity of 2 nd point by adding
  velocities:
   v2 = v1 + v(2 relative to 1)
                                           object 2
            vy (m/s)
                              v2
                                        v(2 relative to 1)
                              v1
                                   object 1
                                                         vx (m/s)




           Relative Angular Velocity
• Angular velocity of a 2 nd line segment relative
  to a 1st line segment
• Compute absolute angular velocity of 2 nd
  segment by adding velocities:

    ω2 = ω1 + ω(2 relative to 1)
                                                 ω(2 relative to 1)
                                   ω2

                  ω1




                                                                      7
Rotation About a Moving Axis
When a point is rotating relative to a moving axis of
  rotation, the absolute velocity of the point is the
  vector sum of:
• the point’s velocity relative to the axis, and
• the velocity of the axis                vaxis
   v2 = vaxis + vt             vt = r ω               v2
                                                point 2

                                          r
                               ω
            axis of rotation
                                              vaxis




             Example Problem #4
 A soccer player kicks a ball 3 different ways:
 1) stands still and contacts the ball with the lower
     limb vertical and swinging forward at 300°/s
 2) same as (1), except he runs forward at 3 m/s
 3) he stands still and contacts the ball with the hip
     flexed 10° and flexing at 300°/s and the knee
     flexed 17.5° and extending at 100°/s
 The length of his thigh and leg are each 45 cm
 What is the linear velocity of the ankle at the time
     of ball contact in each case?




                                                           8
Tools for Measuring Kinematics
• Cinematograpy & Videography
• Motion Capture System
  – measures position
  – can derive all linear & angular quantities
• Goniometer or Electrogoniometer
  – measures angular position
  – can derive angular velocity & acceleration
• Timers (Stopwatch or Electronic)
  – measures timing
  – can derive velocity
• Accelerometer
  – measures linear acceleration
  – can derive linear velocity and displacement




                                                  9

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Lecture 11

  • 1. Linear & Angular Motion (part 2) Objectives: • Learn the relationship between linear and angular velocity for a body in rotation • Learn to compute the tangental and radial acceleration of a body in rotation • Learn how to analyze general motion • Become familiar with methods for measuring kinematic quantities Linear & Angular Velocity The instantaneous linear velocity (v) of a point on a rotating body is: • In a direction tangental to the path of motion • Has a signed magnitude (v) of: v v=rω where: ω • r = radius of rotation r • ω = angular velocity in radian/s ! axis of rotation 1
  • 2. Finding the Tangental Direction • Instantaneous linear velocity directed ±90° from the line segment from the axis of rotation to the point v θ+90° ω (θ – 90°) ω v θ θ ω counterclockwise ω clockwise (ω and v positive) (ω and v negative) Example Problem #1 A quarterback starts to throw with his arm angled 170° with respect to the forward (+x) direction. He accelerates his arm forward (clockwise) at 3000°/s2 He releases the football when his arm is at 120° His arm is 70 cm long. What is the linear velocity of his hand at the instant he releases the football? 2
  • 3. Radial & Tangental Velocity Changes • The linear velocity of a rotating object changes: – along the path of v2 motion (tangental) – perpendicular to the path of motion ∆vradial ∆vtangental (radial) v1 • Thus, it must also v2 accelerate in the ω2 tangental & radial directions ω1 Radial & Tangental Acceleration • The acceleration of a body in angular motion can be resolved into two components: – Tangental: along the path of motion atangental – Radial: a perpendicular to the path of aradial motion a = atangental + aradial α ω 3
  • 4. Tangental Acceleration • Component of acceleration directed along a tangent to the path of motion • Represents a change in linear speed v2 – v1 v2 at = t2 – t1 v1 at • If r is constant: r2 r ω2 – r ω1 at = t2 – t1 ω2 r1 at = r α α in radian/s2 ! ω1 Radial Acceleration • Component of acceleration directed towards the center of curvature • Represents a change in direction v v2 ar = r • If r is constant: ar rω 2 ω ar = r r ar = r ω2 ω in radian/s ! 4
  • 5. Tangental & Radial Directions • Tangental acceleration directed ±90° from the line segment from the axis of rotation to the point • Radial acceleration always directed inward at θ+90° ar ar (θ – 90°) α at α θ θ α counterclockwise α clockwise (α and a t positive) (α and a t negative) Release of a Rotating Object • At the instant that v2 without ar radial acceleration is removed, v2 with ar an object becomes projected in the v1 tangental direction r ω 5
  • 6. Example Problem #2 In problem #1, what is the average acceleration of the hand-and-ball along the path of motion between the start of the throw and the release of the ball? At the instant before the football leaves the hand, what are its linear velocity and acceleration? At the instant after the football leaves the hand, what are its linear velocity and acceleration? If we know that the ball is released from a height of 2.1 m, can we determine how far downfield it can travel? Example Problem #3 Two runners are racing the 200 m. Runner #1 is in lane 1, Runner #2 is in lane 8. The inside radius of the track is 36.8 m. Each lane is 1.1 m wide. If both runners try to run the curve at 9 m/s, how much will each runner need to accelerate in the radial direction? 6
  • 7. Relative Linear Velocity • Apparent velocity of a 2 nd point to an observer at a 1st moving point • Compute absolute velocity of 2 nd point by adding velocities: v2 = v1 + v(2 relative to 1) object 2 vy (m/s) v2 v(2 relative to 1) v1 object 1 vx (m/s) Relative Angular Velocity • Angular velocity of a 2 nd line segment relative to a 1st line segment • Compute absolute angular velocity of 2 nd segment by adding velocities: ω2 = ω1 + ω(2 relative to 1) ω(2 relative to 1) ω2 ω1 7
  • 8. Rotation About a Moving Axis When a point is rotating relative to a moving axis of rotation, the absolute velocity of the point is the vector sum of: • the point’s velocity relative to the axis, and • the velocity of the axis vaxis v2 = vaxis + vt vt = r ω v2 point 2 r ω axis of rotation vaxis Example Problem #4 A soccer player kicks a ball 3 different ways: 1) stands still and contacts the ball with the lower limb vertical and swinging forward at 300°/s 2) same as (1), except he runs forward at 3 m/s 3) he stands still and contacts the ball with the hip flexed 10° and flexing at 300°/s and the knee flexed 17.5° and extending at 100°/s The length of his thigh and leg are each 45 cm What is the linear velocity of the ankle at the time of ball contact in each case? 8
  • 9. Tools for Measuring Kinematics • Cinematograpy & Videography • Motion Capture System – measures position – can derive all linear & angular quantities • Goniometer or Electrogoniometer – measures angular position – can derive angular velocity & acceleration • Timers (Stopwatch or Electronic) – measures timing – can derive velocity • Accelerometer – measures linear acceleration – can derive linear velocity and displacement 9