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Ch11-1 Torque Chapter 11: Rotational Dynamics and Static Equilibrium  CCW +

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Presentation on theme: "Ch11-1 Torque Chapter 11: Rotational Dynamics and Static Equilibrium  CCW +"— Presentation transcript:

1 Ch11-1 Torque Chapter 11: Rotational Dynamics and Static Equilibrium  CCW +

2 Applying a Torque

3 Ct1: You are using a wrench and trying to loosen a rusty nut. Which of the arrangements shown is least effective in loosening the nut? AB CD

4 Ch11-1 Torque  = rF  = rFsin Chapter 11: Rotational Dynamics and Static Equilibrium

5 Torque = moment arm x force = r  F = rsinF Chapter 11: Rotational Dynamics and Static Equilibrium line of action of the force moment arm The moment arm is the perpendicular distance from rotation axis to the line of action of the force.

6 P11.2 (p.350)

7 Ch11-2 Torque and Angular Acceleration  = I Torques summed about fixed axis O. P11.15 (p.351) Chapter 11: Rotational Dynamics and Static Equilibrium  CCW +

8 CT2: Two wheels with fixed hubs, each having a mass of 1 kg, start from rest, and forces are applied as shown. Assume the hubs and spokes are massless, so that the rotational inertia is I = mR 2. In order to impart identical angular accelerations, how large must F 2 be? A N B. 0.5 N C. 1 N D. 2 N E. 4 N

9 Ch11-3 Zero Torque and Static Equilibrium F = 0 and  = 0 P11.22 (p.351) Chapter 11: Rotational Dynamics and Static Equilibrium  CCW + 

10 CT3: P11.22c If the mass of the teeter-totter were doubled, the answers to parts a and b for the position of the applied force would A. double. B. halve. C. stay the same.

11 P11.31 (p.352)

12 Ch11-4 Center of Mass and Balance Near the Earth, the center of mass is the balance point of an object. Chapter 11: Rotational Dynamics and Static Equilibrium

13 Ch11-5 Dynamic Applications of Torque We can finally relax the simplification that a pulley is massless. P11.44 (p.353) Chapter 11: Rotational Dynamics and Static Equilibrium

14 CT4: P11.44a The 25N tension is A. greater than the tension on the other side. B. less than the tension on the other side. C. the same as the tension on the other side.

15 Ch11-6 Angular Momentum p = mv (kgm/s) L = I (fixed axis) (kgm 2 /s) F = p/t  = L/t P11.55 (p.353) Chapter 11: Rotational Dynamics and Static Equilibrium    

16 Ch11-7 Conservation of Angular Momentum If F ext = 0, then p tot is conserved If  = 0, then L tot is conserved P11.63 (p.354) Chapter 11: Rotational Dynamics and Static Equilibrium  

17 Ch11-8 Rotational Work and Power W = Fx =  (one dimension or fixed axis) W = K Power = W/t = /t =  P11.68 (p.354) Chapter 11: Rotational Dynamics and Static Equilibrium


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