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F acceleration, a angular acceleration, m/sec 2 radians/sec 2 or degrees/sec 2 ve seen our “equations of mot omplemented by descriptions o spinning and rotation: Recall: inear) momentum: mv = consta m/sec inear) momentum: I = consta radians/sec

F acceleration, a angular acceleration, m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

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Page 1: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

F acceleration, a

angular acceleration,

m/sec2

radians/sec2

ordegrees/sec2

We’ve seen our “equations of motion”complemented by descriptions of

spinning and rotation:

Recall:

(linear) momentum: mv = constant

m/sec

(linear) momentum: I = constantradians/sec

Page 2: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

Fgravity

The moon is always “falling”, but

- Never changes speed:

No increase inKinetic Energy!

- Never gets any closer to the earth:

No decrease inPotential Energy!

Page 3: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

Center of mass/ center of balance

Page 4: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of
Page 5: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

Fgrav

Fgrav

FgravFgrav

N

N

N

N

Page 6: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of
Page 7: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of
Page 8: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of
Page 9: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

A tricycle provides a large baseand ordinarily a rider’s center of massis comfortably within its boundaries.

f

v v

f vBut a child’s inertiacan carry them tooeasily outside that

bounds on a fast turn.

Page 10: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

Note the low center-of-mass for riders of a Big Wheel

Page 11: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

What helps keep a bicycle steady?

Page 12: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of
Page 13: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

This unicyle is being ridden past you to the left.By the right-hand-rule, the angular momentumof the wheel points

A. right. B. left.C. down. D. up.E. into the screen.F. out of the screen.

Page 14: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

2

iirmIrotational mass

somewhat large since some body parts are held

out at large distances ri from the center.

now all body parts

are held in at small ri from the center.

I11 = I22

Page 15: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of
Page 16: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of
Page 17: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

This motorcyclist is A. falling down.B. making a left turn.C. making a right turn.

Page 18: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

W

N

f

N

f

total forcefrom road surface on motorcycle

Page 19: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

N

f

But what about the torque gravity applies?

The total surface forces are not off-centered at allso produce no net torque of their own!

Page 20: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

If this wheel started to tip to the left:

This would be due to a torque(applied by gravity)

By the right-hand-rule, this torque points in what direction?

A. right. B. left.C. down. D. up.E. into the screen.F. out of the screen.

Page 21: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

A torque of course produces a change in angular momentum:

This changewill be inthe directionof the torque(out towardsyou in thispicture). '

the new angular momentum

What does this mean?

This gyroscopic precession will actually steer the wheel naturally to the left!

Page 22: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

ballballcuecuevm vm

5500

Head-on elastic collisions:

ballcuev v

5

V

of equal masses:

What happens in a head-on collisionwith a much heavier mass?

Page 23: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

V

Page 24: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

V ~V

Page 25: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

What about the (more common) glancing blow?

Remember:contact forces are NORMAL forces!

To understand what effect this has, consider bouncing a ball off the ground…

Page 26: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

A glancing blow with the ground is like partly traveling straight down

into it and, at the same time, trying to

travel past it.

This part of its motion(the downward component of its velocity) is reversedby the collision, just like a head-on collision event.

The horizontalcomponent of its

motion is unaffected!

Page 27: F acceleration, a  angular acceleration,  m/sec 2 radians/sec 2 or degrees/sec 2 We’ve seen our “equations of motion” complemented by descriptions of

F. With the fingers of your right hand curled in the direction of the rotating wheel, your thumb will point out of the screen.

B. He is leaning to turn to his left.

F. out of the screen.

The direction a torque twists is defined by the same right-hand rule. When screwing inan ordinary (right-hand threaded) screw, with screw- driver in right hand, yourfingers curl in the directionyou’re twisting, and your thumbpoints in the direction you’re driving the screw (the directionof the torque).

Sure, the initial angular momentum of the spinning wheel is to the left. But the torque that’s trying to tip the wheel is rotating it so that the top of the wheel falls over to the left…a counter-clockwise twist of thetop over the bottom edge which is against the ground.