Rotational inertia (moment of inertia)

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1 Rotational inertia (moment of inertia) Define rotational inertia (moment of inertia) to be I = Σ m i r i 2 or r i : the perpendicular distance between m i and the given rotation axis m 1 m 2 x 1 x 2 Moment of inertia

2 Rotational inertia (moment of inertia) Hoop rotating about a central axis Define rotational inertia (moment of inertia) to be r i : the perpendicular dist. between m i and the rotation axis How is the mass distributed on the hoop? >>>> dm/m = rdθ/2πr or dm = ρ r dθ, where ρ = M/2πr r = a Moment of inertia I

3 Rotational inertia involves not only the mass but also the distribution of mass for continuous masses Calculating the rotational inertia

4 Parallel-Axis theorem If we know the rotational inertia of a body about any axis that passes through its center-of-mass, we can find its rotational inertia about any other axis parallel to that axis with the parallel axis theorem I = I c.m. + M h 2 h: the perpendicular distance between the two axes

5 z y Consider a standard blackboard eraser. Rotation along which axis would it have the greatest moment of inertia I? x 1) x 2) y 3) z 4) All have the same I Hint: Look for largest amount of mass away from the axis.

6 Newton s Second Law for Rotation I: rotational inertia α: angular acceleration Compare to the linear equation:

7 Sample Problem 10-8 This figure shows a uniform disk, with mass M = 2.5 kg and radius R = 20 cm, mounted on a fixed horizontal axle. A block with mass m = 1.2 kg hangs from a massless cord that is wrapped around the rim of the disk. Find the acceleration of the falling block, the angular acceleration of the disk, and the tension in the cord. Note: R = 20 cm = 0.2 m y a

8 This figure shows a uniform disk, with mass M=2.5kg and radius R = 20 cm, mounted on a fixed horizontal axle. A block with mass m = 1.2 kg hangs from a massless cord that is wrapped around the rim of the disk. Find the acceleration of the falling block, the angular acceleration of the disk, and the tension in the cord. The key points are following: For the block: T mg = ma (1) For the pulley: τ = I α RT = (1/2)MR 2 α (2) acceleration a of the block is equal to a t at the rim of the pulley a = a t = α R (3) Three equations and three unknowns: a, α, T, so a unique solution exists. a y

9 Sample Problem This figure shows a uniform disk, with mass M=2.5kg and radius R = 20 cm, mounted on a fixed horizontal axle. A block with mass m = 1.2 kg hangs from a massless cord that is wrapped around the rim of the disk. Find the acceleration of the falling block, the angular acceleration of the disk, and the tension in the cord. Equations 2&3: T = (1/2)Ma t Substitute a t /α for R Equations 2&3 and 1: a = αr = (Ma)/2m g Equations 1,3 and 2: a = αr = g MR α/2m Eqn 1: a = T/m g a y

10 Sample Problem This figure shows a uniform disk, with mass M=2.5kg and radius R = 20 cm, mounted on a fixed horizontal axle. A block with mass m = 1.2 kg hangs from a massless cord that is wrapped around the rim of the disk. Find the acceleration of the falling block, the angular acceleration of the disk, and the tension in the cord. Then, T = 1/2Ma = 6.0N y and, α = a/r = 24 rad/s 2 a

11 Work and Rotational Kinetic Energy Work-kinetic energy theorem: W = ΔK = K f K i ΔK = ½ I ω 2 f ½ I ω 2 i (if there is only rotation) Work done (compare to ) if τ is constant, W = τ (θ f θ i ) Power P = dw/dt P =τ dθ/dt = τ ω. compare to P = F v

12 Summary -- Translation - Rotation translational motion Quantity Rotational motion x Position θ Δx Displacement Δθ v = dx/dt Velocity ω = dθ/dt a = dv/dt Acceleration α m Mass Inertia I F = ma Newton s second law Work τ = r x F K = ½ mv 2 Kinetic energy K = ½ Iω 2 Power (constant F or ) P = τω

13 The Kinetic Energy of Rolling View the rolling as pure rotation around P, the kinetic energy K = ½ I P ω 2 parallel axis theorem: I p = I com +MR 2 so K = ½ I com ω 2 + ½ MR 2 ω 2 since v com = ωr K = ½ I com ω 2 + ½ M(v com ) 2 ½ I com ω 2 : due to the object s rotation about its center of mass ½ M(v com ) 2 : due to the translational motion of its center of mass

14 Chapter 11: Rolling, Torque, and Angular Momentum For an object rolling smoothly, the motion of the center of mass is pure translational. s = θ R v com = ds/dt = d(θ R)/dt = ωr v com = ωr

15 Rolling viewed as a combination of pure rotation and pure translation Rolling viewed as pure rotation v top = (ω)(2r) = 2 v com Different views, same conclusion

16 Sample Problem: A uniform solid cylindrical disk, of mass M = 1.4 kg and radius R = 8.5 cm, rolls smoothly across a horizontal table at a speed of 15 cm/s. What is its kinetic energy K? v c.m. = 0.15m/s I disk =1/2MR 2 = (0.5)(1.4kg)(0.085m) 2 = 5.058x10 3 kg m 2 ω = v/r = (0.15m/s)/0.085m = rad/s

17 Angular momentum Angular momentum with respect to point O for a particle of mass m and linear momentum p is defined as: Compare to the linear case p = mv direction: right-hand rule magnitude:

18 The angular momentum of a rigid body rotating about a fixed axis Consider a simple case, a mass m rotating about a fixed axis z: = r m v sin90 o = r m r ω = mr 2 ω = I ω v r z y x In general, the angular momentum of a rigid body rotating about a fixed axis is L = I ω L : angular momentum (group or body) along the rotation axis : angular momentum (particle) along the rotation axis I : moment of inertia about the same axis

19 Sample Problem Particles 1, 2, 3, 4, and 5 have the same mass and speed as shown in the figure. Particles 1 & 2 move around O in opposite directions. Particles 3, 4, and 5 move towards or away from O as shown. 2r 2r r r Which of the particles has the smallest magnitude angular momentum? 1) 1 2) 2 3) 3 4) 4 5) 5 6) all have the same l

20 Sample Problem Particles 1, 2, 3, 4, and 5 have the same mass and speed as shown in the figure. Particles 1 & 2 move around O in opposite directions. Particles 3, 4, and 5 move towards or away from O as shown. 2r 2r r r Φ = 0 o for 5. => l = 0 Which of the particles has the smallest magnitude angular momentum? 1) 1 2) 2 3) 3 4) 4 5) 5 6) all have the same l

21 Newton s Second Law in Angular Form Let be the vector sum of all the torques acting on the object. Net external torque equals to the time rate change of the system s total angular momentum

22 Conservation of Angular Momentum If the net external torque acting on a system is zero, the angular momentum of the system is conserved. If then For a rigid body rotating around a fixed axis, ( L = I ) the conservation of angular momentum can be written as I i i = I f f

23 Some examples involving conservation of angular momentum The spinning volunteer L f = L i => I f f = I i i

24 Angular momentum is conserved L i is in the spinning wheel Now exert a torque to flip its rotation. L f, wheel = L i. Conservation of Angular momentum means that the person must now acquire an angular momentum. L f, person = +2L i so that L f = L f, person + L f, wheel =+2L i + L i = L i.

25 More examples The springboard diver Spacecraft orientation

26 Problem Ring of R 1 (=R 2 /2) and R 2 (=0.8m), Mass m 2 = 8.00kg. i = 8.00 rad/s. Cat m 1 = 2kg. Find kinetic energy change when cat walks from outer radius to inner radius.

27 Initial Momentum Problem Ring of R 1 (=R 2 /2) and R 2 (=0.8m), Mass m 2 = 8.00kg. i = 8.00 rad/s. Cat m 1 = 2kg. Find kinetic energy change when cat walks from outer radius to inner radius.

28 Problem Ring of R 1 (=R 2 /2) and R 2 (=0.8m), Mass m 2 = 8.00kg. i = 8.00 rad/s. Cat m 1 = 2kg. Find kinetic energy change when cat walks from outer radius to inner radius. Final Momentum

29 Problem 11-66

30 Problem Ring of R 1 (=R 2 /2) and R 2 (=0.8m), Mass m 2 = 8.00kg. i = 8.00 rad/s. Cat m 1 = 2kg. Find kinetic energy change when cat walks from outer radius to inner radius. Initial Kinetic energy K i is:

31 Torque and Angular Momentum Torque is the time rate of change of angular momentum.

32 Precession Torque is the time rate of change of angular momentum. mg θ r Falling due to torque about the pivot point. τ = rfsinθ = rmg sinθ Falling causes angular momentum about the pivot point (along y-axis).

33 Precession Torque is the time rate of change of angular momentum. mg θ r Falling due to torque about the pivot point. τ = rfsinθ = rmg sinθ Falling causes angular momentum about the pivot point (along y-axis). Now set the gyroscope in motion L=I (along x-axis) L is fixed by the spinning, so the torque can only change the direction of L

34 Precession Rate Torque is the time rate of change of angular momentum. mg θ r Falling due to torque about the pivot point. Falling causes angular momentum about the pivot point (along y-axis). (Precession along z-axis)

35 Precession Rate Torque is the time rate of change of angular momentum. mg θ r Nuclei have intrinsic angular momentum. This effect is at the core of MRI, which is tuned to pick up the intrinsic angular momentum of the proton in hydrogen. (Precession along z-axis)

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Team: Rotational Motion Rotational motion is everywhere. When you push a door, it rotates. When you pedal a bike, the wheel rotates. When you start an engine, many parts rotate. Electrons rotate in an

Physics 1120: Work & Energy Solutions

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If something is spinning, it moves more quickly if it. d is farther from the center of rotation. For instance, θ

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Angular acceleration α

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TORQUE. Objective: To measure the angular motion of a disk, which rotates due to the application of a force.

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Conservation of Angular Momentum

Conservation of Angular Momentum If the net external torque on a system is zero, the angular momentum is conserved. The most interesting consequences occur in systems that are able to change shape: So

Midterm Solutions. mvr = ω f (I wheel + I bullet ) = ω f 2 MR2 + mr 2 ) ω f = v R. 1 + M 2m

Midterm Solutions I) A bullet of mass m moving at horizontal velocity v strikes and sticks to the rim of a wheel a solid disc) of mass M, radius R, anchored at its center but free to rotate i) Which of

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Chapter 10 Dynamics of Rotational Motion PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by James Pazun Modified by P. Lam 5_31_2012 Goals for Chapter

PHY231 Section 1, Form B March 22, 2012

1. A car enters a horizontal, curved roadbed of radius 50 m. The coefficient of static friction between the tires and the roadbed is 0.20. What is the maximum speed with which the car can safely negotiate

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Single and Double plane pendulum Gabriela González 1 Introduction We will write down equations of motion for a single and a double plane pendulum, following Newton s equations, and using Lagrange s equations.

Mechanics Cycle 1 Chapter 13. Chapter 13

Chapter 13 Torque * How Shall a Force be Applied to Start a Rotation? The Torque Formula Systems in Equilibrium: Statics Glimpse of Newton s rotational second law: Q: Review: What causes linear acceleration