2 What Is Rotational Motion? What does a yo-yo have in common with a merry-go-round?How can we describe this type of motion?
3 Linear Motion vs. Rotational Motion Linear motion involves an object moving from one point to another in a straight line.Rotational motion involves an object rotating about an axis.Examples include a merry-go-round, the rotating earth, a spinning skater, a top, and a turning wheel.What causes rotational motion?Does Newton’s second law apply?
4 For every type of linear quantity we have a rotational quantity that does much the same thing : Linear QuantitiesSpeedForceMassMomentumDistanceRotational QuantitiesRotational (Angular) SpeedTorqueRotational InertiaAngular MomentumAngle
5 V=rω Relationship between linear and rotational velocity On a merry-go-round, a rider near the edge travels a greater distance in 1 revolution than one near the center.The outside rider is therefore traveling with a greater linear speed.V=rω
6 A merry-go-round is accelerated at a constant rate of 0 A merry-go-round is accelerated at a constant rate of rev/s2, starting from rest. What is its rotational velocity at the end of 1 min?0.005 rev/s0.03 rev/s0.05 rev/s0.30 rev/s = rev/s20 = 0t = 60 s = 0 + t= 0 + (0.005 rev/s2)(60 s)= 0.30 rev/s
7 How many revolutions does the merry-go-round make in 1 minute? = rev/s20 = 0t = 60 s, = 0.30 rev/s = 0t + 1/2 t2= 0 + 1/2 (0.005 rev/s2)(60 s)2= 9 rev
8 Torque and BalanceWhat causes the merry-go-round to rotate in the first place?What determines whether an object will rotate?If an unbalanced force causes linear motion, what causes rotational motion?
9 Torque and Balance When is a balance balanced? Consider a thin but rigid beam supported by a fulcrum or pivot point.If equal weights are placed at equal distances from the fulcrum, the beam will not tend to rotate: it will be balanced.
10 To balance a weight twice as large as a smaller weight, the smaller weight must be placed twice as far from the fulcrum as the larger weight.Both the weight and the distance from the fulcrum are important.The product of the force and the distance from the fulcrum is called the torque.Torque describes the tendency of a weight to produce a rotation.
11 The distance from the fulcrum to the point of application of the force must be measured in a direction perpendicular to the line of action of the force.This distance iscalled the lever armor moment arm.A longer lever armproduces a greatertorque.For a force F and alever arm l, theresulting torque is:
12 A 50-N force is applied at the end of a wrench handle that is 24 cm long. The force is applied in a direction perpendicular to the handle as shown. What is the torque applied to the nut by the wrench?6 N·cm12 N·cm26 N·cm120 N·cm0.24 m 50 N = 12 N·cm
13 What would the torque be if the force were applied half way up the handle instead of at the end? 6 N·m12 N·m26 N·m120 N·m0.12 m 50 N = 6 N·m
14 When the applied force is not perpendicular to the crowbar, for example, the lever arm is found by drawing the perpendicular line from the fulcrum to the line of action of the force.We call torquesthat producecounterclockwiserotation positive,and torques thatproduceclockwise rotationnegative.
15 Two forces are applied to a merry-go-round with a radius of 1 Two forces are applied to a merry-go-round with a radius of 1.2 m as shown. What is the torque about the axle of the merry-go-round due to the 80-N force?+9.6 N·m-36 N·m+96 N·m1.2 m 80 N = +96 N·m(counterclockwise)
16 What is the torque about the axle of the merry-go-round due to the 50-N force? +60 N·m-60 N·m+120 N·m-120 N·m-(1.2 m 50 N) = -60 N·m(clockwise)
17 What is the net torque acting on the merry-go-round? +36 N·m-36 N·m+96 N·m-60 N·m+126 N·m96 N·m (counterclockwise)60 N·m (clockwise)= +36 N·m (counterclockwise)
18 We want to balance a 3-N weight against a 5-N weight on a beam We want to balance a 3-N weight against a 5-N weight on a beam. The 5-N weight is placed 20 cm to the right of a fulcrum. What is the torque produced by the 5-N weight?+1 N·m-1 N·m+4 N·mF = 5 N = - Fll = 20 cm = 0.2 m = - (5 N)(0.2 m)= -1 N·m
19 How far do we have to place the 3-N weight from the fulcrum to balance the system? 2 cm27 cm33 cm53 cmF = 3 N l = / F = +1 N·m = (+1 N·m) / (3 N)= 0.33 m = 33 cm
20 The center of gravity of an object is the point about which the weight of the object itself exerts no torque.We can locate the center of gravity by finding the point where it balances on a fulcrum.For a more complex object, we locate the center of gravity by suspending theobject from twodifferent points,drawing a line straightdown from the point ofsuspension in eachcase, and locating thepoint of intersection ofthe two lines.
21 Rotational Inertia and Newton’s Second Law In linear motion, net force and mass determine the acceleration of an object.For rotational motion, torque determines the rotational acceleration.The rotational counterpart to mass is rotational inertia or moment of inertia.Just as mass represents the resistance to a change in linear motion, rotational inertia is the resistance of an object to change in its rotational motion.Rotational inertia is related to the mass of the object.It also depends on how the mass is distributed about the axis of rotation.
22 Simplest example: a mass at the end of a light rod A force is applied to the mass in a direction perpendicular to the rod.The rod and mass will begin to rotate about the fixed axis at the other end of the rod.The farther the mass is from the axis, the faster it moves for a given rotational velocity.
23 Simplest example: a mass at the end of a light rod To produce the same rotational acceleration, a mass at the end of the rod must receive a larger linear acceleration than one nearer the axis.It is harder to get the system rotating when the mass is at the end of the rod than when it is nearer to the axis.
24 Rotational Inertia and Newton’s Second Law The resistance to a change in rotational motion depends on:the mass of the object;the square of the distance of the mass from the axis of rotation.For an object with its mass concentrated at a point:Rotational inertia = mass x square of distance from axisI = mr2The total rotational inertia of an object like a merry-go-round can be found by adding the contributions of all the different parts of the object.
25 Rotational Inertia and Newton’s Second Law Newton’s second law for linear motion:Fnet = maNewton’s second law for rotational motion:The net torque acting on an object about a given axis is equal to the rotational inertia of the object about that axis times the rotational acceleration of the object.net = IThe rotational acceleration produced is equal to the torque divided by the rotational inertia.
26 Example: a baton with a mass at both ends Most of the rotational inertia comes from the masses at the ends.A torque can be applied at the center of the rod, producing a rotational acceleration and starting the baton to rotate.If the masses were moved toward the center, the rotational inertia would decrease and the baton would be easier to rotate.
27 Some objects have more rotational inertia than others Objects with mass closer to axis of rotation are easier to rotate, b/c it they have less rotational inertiaIf the mass is farther away from the axis, then object will have more rotational inertia, and will therefore be harder to rotate
28 Two 0.2-kg masses are located at either end of a 1-m long, very light and rigid rod as shown. What is the rotational inertia of this system about an axis through the center of the rod?0.02 kg·m20.05 kg·m20.10 kg·m20.40 kg·m2I = mr2= (0.2 kg)(0.5m)2 x 2= 0.10 kg·m2
29 Conservation of Angular Momentum How do spinning skaters or divers change their rotational velocities?
30 Angular MomentumLinear momentum is mass (inertia) times linear velocity: p = mvAngular momentum is rotational inertia times rotational velocity:L = IAngular momentum may also be called rotational momentum.A bowling ball spinning slowly might have the same angular momentum as a baseball spinning much more rapidly, because of the larger rotational inertia I of the bowling ball.
31 Conservation of Angular Momentum Angular momentum is conserved if the net external torque acting on the system is zero.
32 Angular momentum is conserved by changing the angular velocity When the masses are brought in closer to the student’s body, his rotational velocity increases to compensate for the decrease in rotational inertia.He spins faster when the masses are held close to his body, and he spins more slowly when his arms are outstretched.
33 Kepler’s Second LawKepler’s second law says that the radius line from the sun to the planet sweeps out equal areas in equal times.The planet moves faster in its elliptical orbit when it is nearer to the sun than when it is farther from the sun.
34 Kepler’s Second Law This is due to conservation of angular momentum. The gravitational force acting on the planet produces no torque about an axis through the sun because the lever arm is zero: the force’s line of action passes through the sun.
35 Kepler’s Second LawWhen the planet moves nearer to the sun, its rotational inertia about the sun decreases.To conserve angular momentum, the rotational velocity of the planet about the sun must increase.
36 Riding a bicycle and other amazing feats Why does a bicycle remain upright when it is moving but promptly falls over when not moving?
37 Angular momentum is a vector The direction of the rotational-velocity vector is given by the right-hand rule.The direction of the angular-momentum vector is the same as the rotational velocity.
38 Angular momentum and bicycles The wheels have angular momentum when the bicycle is moving.For straight line motion, the direction of the angular-momentum vector is the same for both wheels and is horizontal.To tip the bike over, the direction of the vector must change, requiring a torque.
39 Angular momentum and bicycles If the bike is not perfectly upright, a gravitational torque acts about the line of contact of the tires with the road.As the bike begins to fall, it acquires a rotational velocity and angularmomentum aboutthis axis.If the bike tilts to theleft, the change inangular momentumpoints straight back.
40 Angular momentum and bicycles If the bike is standing still, the gravitational torque causes the bike to fall.
41 Angular momentum and bicycles When the bike is moving, the change in angular momentum caused by the gravitational torque adds to the angular momentum already present from the rotating tires.This causes achange in thedirection of thetotal-angularmomentum vectorwhich can beaccommodated byturning the wheel.
42 A student holds a spinning bicycle wheel while sitting on a stool that is free to rotate. What happens if the wheel is turned upside down?To conserve angular momentum, the original direction of the angular-momentum vector must be maintained.
43 A student holds a spinning bicycle wheel while sitting on a stool that is free to rotate. What happens if the wheel is turned upside down?The angular momentum of the student and stool, +Ls, adds to that of the (flipped) wheel, -Lw, to yield the direction and magnitude of the original angular momentum +Lw.
44 upward from plane of wheel A student sits on a stool holding a bicycle wheel with a rotational velocity of 5 rev/s about a vertical axis. The rotational inertia of the wheel is 2 kg·m2 about its center and the rotational inertia of the student and wheel and platform about the rotational axis of the platform is 6 kg·m2. What is the initial angular momentum of the system?10 kg·m2/s upward25 kg·m2/s downward25 kg·m2/s upward50 kg·m2/s downwardL = I = (2 kg·m2)(5 rev/s)= 10 kg·m2/supward from plane of wheel
45 = L / I = (20 kg·m2/s) / (6 kg·m2) = 3.33 rad/s If the student flips the axis of the wheel, reversing the direction of its angular-momentum vector, what is the rotational velocity of the student and stool about their axis after the wheel is flipped?1.67 rad/s3.33 rad/s60 rad/s120 rad/s = L / I = (20 kg·m2/s) / (6 kg·m2)= 3.33 rad/sin direction of original angular velocity