10/10/2012PHY 113 A Fall 2012 -- Lecture 171 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 17: Chapter 10 – rotational motion 1.Angular.

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10/10/2012PHY 113 A Fall Lecture 171 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 17: Chapter 10 – rotational motion 1.Angular variables 2.Rotational energy 3.Moment of inertia

10/10/2012 PHY 113 A Fall Lecture 172

10/10/2012PHY 113 A Fall Lecture 173 Angular motion angular “displacement”   (t) angular “velocity”  angular “acceleration”  “natural” unit == 1 radian Relation to linear variables: s  = r (  f -  i ) v  = r  a  = r  s

10/10/2012PHY 113 A Fall Lecture 174 Special case of constant angular acceleration:  =  0 :  t  =  i +   t  t  =  i +  i t +  ½   t 2 (  t    i    t  -  i   r1r1 v 1 =r 1  v 2 =r 2  r2r2

10/10/2012PHY 113 A Fall Lecture 175 A wheel is initially rotating at a rate of f=30 rev/sec. R

10/10/2012PHY 113 A Fall Lecture 176 A wheel is initially rotating at a rate of f=30 rev/sec. Because of a constant angular deceleration, the wheel comes to rest in 3 seconds. R

10/10/2012PHY 113 A Fall Lecture 177 Example: Compact disc motion In a compact disk, each spot on the disk passes the laser-lens system at a constant linear speed of v  = 1.3 m/s.  1 =v  /r 1 =56.5 rad/s  2 =v  /r 2 =22.4 rad/s What is the average angular acceleration of the CD over the time interval  t=4473 s as the spot moves from the inner to outer radii?  = (  2 -  1 )/  t = rad/s 2 11 22

10/10/2012PHY 113 A Fall Lecture 178 Object rotating with constant angular velocity (  = 0)  v=0 v=R  Kinetic energy associated with rotation: “moment of inertia” R

10/10/2012PHY 113 A Fall Lecture 179 Moment of inertia: iclicker exercise: Which case has the larger I? A. a B. b

10/10/2012PHY 113 A Fall Lecture 1710 Moment of inertia:

10/10/2012PHY 113 A Fall Lecture 1711 Note that the moment of inertia depends on both a)The position of the rotational axis b)The direction of rotation mm dd I=2md 2 mm dd I=m(2d) 2 =4md 2

10/10/2012PHY 113 A Fall Lecture 1712 iclicker question: Suppose each of the following objects each has the same total mass M and outer radius R and each is rotating counter- clockwise at an constant angular velocity of  =3 rad/s. Which object has the greater kinetic energy? (a) (Solid disk) (b) (circular ring)

10/10/2012PHY 113 A Fall Lecture 1713 Various moments of inertia: solid cylinder: I=1/2 MR 2 solid sphere: I=2/5 MR 2 solid rod: I=1/3 MR 2 R R R

10/10/2012PHY 113 A Fall Lecture 1714 Calculation of moment of inertia: Example -- moment of inertia of solid rod through an axis perpendicular rod and passing through center: R

10/10/2012PHY 113 A Fall Lecture 1715 Note that any solid object has 3 moments of inertia; some times two or more can be equal j i k iclicker exercise: Which moment of inertia is the smallest? (A) i (B) j (C) k

10/10/2012PHY 113 A Fall Lecture 1716 iclicker exercise: Three round balls, each having a mass M and radius R, start from rest at the top of the incline. After they are released, they roll without slipping down the incline. Which ball will reach the bottom first? A B C

10/10/2012PHY 113 A Fall Lecture 1717

10/10/2012PHY 113 A Fall Lecture 1718 iclicker exercise: Three round balls, each having a mass M and radius R, start from rest at the top of the incline. After they are released, they roll without slipping down the incline. Which ball will reach the bottom first? A B C