. Why doesn't an egg break when it falls into a pile of feathers? Isn't the pile of feathers exerting the same force on it (perhaps 1000 newtons) that a table would if it were to hit that table?
The egg doesn't break because the feathers exert a much smaller force on the egg than the table would. The feathers can move so when the egg first hits them, the feathers don't have to stop the egg so quickly. To keep the egg from penetrating into the table, the table has to stop the egg's descent in about a thousandth of a second. That required a huge upward force on the egg of perhaps 1000 N. This large upward force, exerted on one small point of the egg, breaks the egg. But when the egg hits the feathers, the feathers can stop the egg's descent leisurely in about a tenth of a second. They only have to push upward on the egg with a smaller force of perhaps 10 N. This modest force, exerted on many points of the egg, shouldn't break the egg. During this tenth of a second, the feathers and the egg will both move downward and the egg will come to a stop well below the place at which it first touched the feathers.
. Can you give me an example of when the angular acceleration is in a different direction from the torque applied?
When an object isn't symmetric, it can rotate in very peculiar ways. If you throw a tennis racket into the air so that it is spinning about an axis that isn't along the handle or at right angles to the handle, it will wobble in flight. Its axis of rotation will actually change with time as it wobbles. If you were to exert a torque on this wobbling tennis racket, its angular acceleration wouldn't necessarily be along the direction of the torque.
. Given a lever long enough, could you move the world?
Yes. Of course, you would need a fixed pivot about which to work and that might be hard to find. But you could do work on the world with your lever. If the arm you were dealing with was long enough, you could do that work with a small force exerted over a very, very long distance. The lever would then do this work on the world with a very, very large force exerted over a small distance.
. How can cats turn their bodies around to land on their feet if they fall and how can people do tricks in the air when they are skydiving if you're supposed to "keep doing what you've been doing" when you leave the ground?
Cats manage to twist themselves around by exerting torques within their own bodies. They aren't rigid, so that one half of the cat can exert a torque on the other half and vice versa. Even though the overall cat doesn't change its rotation, parts of the cat change their individual rotations and the cat manages to reorient itself. It goes from not rotating but upside down to not rotating but right side up. Overall, it never had any angular velocity. As for skydiving, that is mostly a matter of torques from the air. As you fall, the air pushes on you and can exert torques on you about your center of mass. The result is rotation.
. Is moment of inertia determined only by mass, as inertia is in translational motion?
No, moment of inertia embodies both mass and its distribution about the axis of rotation. The more of the mass that is located far from the axis of rotation, the larger the moment of inertia. For example, a ball of dough is much easier to spin than a disk-shaped pizza, because the latter has its mass far from the axis of rotation.
. Shouldn't the seesaw be completely horizontal in order to be balanced? How can it be balanced if it's not horizontal?
A balanced seesaw is simply one that isn't experiencing any torque—the net torque on it is zero. Because there is no torque on it, it isn't undergoing any angular acceleration and its angular velocity is constant. If it happens to be horizontal and motionless, then it will stay that way. But it could also be tilted or even rotating at a steady rate.
. What exactly are angular speed and angular velocity?
Angular speed is the measure of how quickly an object is turning. For example, an object that is spinning once each second has an angular speed of "1 rotation-per-second," or equivalently "360 degrees-per-second." Angular velocity is a combination of angular speed and the direction of the rotation. For example, a clock lying on its back and facing upward has a minute hand with an angular velocity of "1 rotation-per-hour in the downward direction." The downward direction reflects the fact that the minute hand pivots about a vertical axis and that your right hand thumb would point downward if you were to curl your fingers in the direction of the minute hand's rotation.
. What is the difference between right and left hand rules?
The rule that's used in the mechanics of rotation is always the right hand rule and that's important. It represents a choice made long ago about how to describe an object's rotation. Having made that choice, it says that the minute hand of a clock (which naturally rotates clockwise) points into the clock. You know that because if you curl the fingers of your right hand in the direction that the minute hand is turning, your extended thumb will point into the clock. There is no left hand rule because that was not the choice made long ago.
. When a lacrosse stick acts as a lever, does it convert a big force to a small one or vice versa?
The lacrosse stick converts a big force into a small one. As you flip the stick, you do work on it—you push part of it forward while that part moves forward. You use a large force and the place on which you push moves forward a small distance. The stick, in turn, does work on the ball. It exerts a small force on the ball but moves that ball through a large distance. The products of force times distance are essentially equal (the stick itself takes some of the energy). The result is a very fast moving lacrosse ball that sails across the field.
. When you exert a torque on a merry-go-round, how does it exert one on you? I have to exert a lot of torque to get it going but it doesn't feel like torque is being exerted back on me.
When you spin a merry-go-round, you exert a torque on it and it exerts a torque back on you. If you were free to rotate, this torque on you would be quite apparent. Suppose that the merry-go-round was located on an ice skating rink and that you were attached to the central pivot of the merry-go-round by a strap that went around your waist. As you spun the merry-go-round clockwise, you would begin to spin counter-clockwise. In fact, because your moment of inertia is much smaller than that of the merry-go-round, you would experience a much larger angular acceleration and would end up spinning much faster than merry-go-round. The reason that you don't rotate like this after spinning a playground merry-go-round is that your feet touch the ground. As the merry-go-round exerts its torque back on you, you exert that same torque on the ground. The result is that the earth undergoes angular acceleration in the opposite direction from that of the merry-go-round. Because the earth's moment of inertia is so huge, you can't tell that it undergoes angular acceleration at all. It really does, just as the earth undergoes acceleration when you jump-you push down hard and the earth as it pushes up hard on you and you both accelerate away from one another. Since the earth is much more massive than you are, it doesn't accelerate nearly as much as you do.