Essentials of Physics- PHYS 101

Lectures 8/9

A joke a day keeps the doctor away

Review of exam

An Example "Physics in the Real World" Report

Review

Torques

Torques and Simple Machines

Centripital Force

Weigh the Earth

Weightlessness

Gravitational Fields

Projectile Motion

Work-Energy Relationship for Satellites

Review of Exam

Example "Physics in the Real World" Report

Review

Why would the egg laid by a cliff bird be so pointy?

Why does a drag racer look so funny?

Not them the car!

It is built extremely long in order to get the largest rotational inertia with the least mass. You can see why this is important below. Later we will discuss what causes the wheelie problem in the first place. You can also understand why the front wheels are so wimpy looking by considering their own rotational inertia.

Torques

Why is it harder to hold something at shoulder height with your arm straight than with it bent? The weight of the object certainly doesn’t depend on how close it is to your body.

That is true, but the torque does.

Torque is the rotational motion counterpart of force.

Just like a net force will change an object’s linear motion, applying a net torque will change an object’s rotational motion.

Torque is different from force in the same way that rotational inertia is different from linear inertia. Torque and rotational inertia both depend on the distance to the axis of rotation. For torque the distance between the axis of rotation and an applied force is called the lever arm.

Torque = lever arm x force

When the net torque acting on something is zero there will be no change in its rotational motion. This is the rotational motion equivalent to Newton's first law.

Two children can balance a seesaw when the weight of each produces an equal torque about the pivot in opposite directions (clockwise and counter clockwise). They can do this even when they have very different weights since they can adjust each lever arm (where they sit related to the pivot) to compensate for the difference in the forces they exert. How about a kid with no friends? He can still use a seesaw! (there's hope for the lonely...)

Torque and Simple Machines

You might get a bright idea from thinking about kids on a seesaw. If a small child can balance a large child by moving farther from the pivot point (fulcrum) then you could lift the large child using a very small force if you pushed down on the seesaw far enough away from the fulcrum. Congratulations! You just invented a machine called the lever! A machine is a devise that multiplies a force and/or changes the direction of the force.

Oops, your ambitious buddy overheard you discussing your invention and has just run off to patent the lever as a way to amplify energy. He saw how easily you lifted the large child and reasons that surely the lever allowed you to increase the Potential Energy of the child by more than the amount of work you did. Are you worried that your so-called friend will make millions off your invention in this way and leave you out in the cold?

Think of all the deep questions that you can answer now that you know about Torque.

The torque about the axle can cause either of two rotations. Either the wheels rotate about the axle or else the car rotates about the axle.

Most people prefer to have the wheels rotate, but as the torque is increased in order to get a huge acceleration at the start that can be a challenge. Although the wheels have much less rotational inertia than the car they are still very hard to accelerate because rolling forward is resisted by the linear inertia of the entire car.

Centripital Force – “And now for something completely different!”

Let’s think back to our discussions of inertia. We said that an object will travel forever at the same velocity (same speed in a straight line) unless a net force acts on the object. What does this tell us about an object that is moving in a circle?

An object moving in a circle is always accelerating (changing velocity but not speed) and therefore always has a net force acting on it. This force must be directed towards the center of the circle. Any force that is directed towards a fixed center is a Centripetal ("center-seeking") Force.

If I whirl a bucket on the end of a string I am constantly pulling towards the center, supplying a centripetal force, in order to cause the bucket to move in a circular path.

Remember your buddy who we shrunk and wasn’t so smart? Well you decided not to re-enlarge him after all and now he’s going for a ride in the bucket. Your buddy is terrified that he will fall out while the bucket is upside-down. He keeps screaming that he wants you to slow down. Do you think that would really be in his best interest?

Once you finally let your buddy out of the bucket (and reluctantly re-enlarge him after letting his temper cool down) you ask him what it was like in the bucket. He describes feeling very heavy during the times when you spun the bucket fast and lighter when you slowed it down.

His conclusion is that a centrifugal force was pulling him towards the bottom of the bucket. You, however, remember from your physics class that there really is no centrifugal force. The combination of his inertia and the bucket pushing him into a circular path create a situation that is almost indistinguishable from gravity for your buddy in the bucket.

For another take on centrifugal forces, think of riding in a car when the car suddenly lurches left to avoid a pedestrian. During this process your upper body and head feel as if they are pushed to the right. In reality, they lack the centripital (center-seeking) force needed to make them move left with the car. Their inertia before the car veers has them going in a straight line. Thus, you seem to feel a centrifugal (outwards) force when the car veers. This is the basis for artificial gravity.

Weigh the Earth

So let's solve this equation (Law) for m2. First multiply both sides by d2. Then divide both sides by m1 and G, leaving:

Weightlessness

Say that astronauts are orbiting the Earth at about 200 miles (320,000 meters) above the surface. The Earth's radius is 6,370,000m, so the astronauts are 6,690,000 meters above the center of the Earth.

The increase in distance from the Earth's center is:

6,690,000/6,370,000 = 1.05

or about 5%. Does this result in a significant decrease in "g" in space? (remember, "g" is the acceleration due to gravity at the Earth's surface.)

What about when we drop or accelerate upwards in an elevator?

What does Newton's Law have to say about these situations?

Gravitational Fields

We represent "action at a distance" forces like gravity, electricity and magnetism using the notion of the "field."

Definition: A field arrow gives the direction of the force. Either the length of the arrow or the density of arrows represents the field's "strength" (force it can impart on a given unit).

How do we draw gravity field arrows for the Earth?

Projectile Motion

We call this motion (ball rolling of the end of table) projectile motion. It describes the motion of baseballs, cannonballs, divers at the pool, etc.

What do we notice about our projectile motion experiment?

This information can be used to launch satellites!

Work-Energy Relationship for Satellites

What is the energy situation of a satellite in orbit?

Circular orbit:

Elliptical orbit:

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