In order to find the distance the wheel travels, we need a way to convert angular displacement to linear displacement. We know that the circumference of a circle (or a wheel, in this case) is . This means that in one rotation, the wheel would travel a distance equal to its circumference.

Distance of one rotation equals: .

Since the wheel travels  rotations, the total distance that the wheel travels will be equal to the distance traveled by one rotation multiplied by the number of rotations.

Distance of rotations equals:

We use the equation for centripetal force to find the radius:

Since the string ties the ball to the axis, the force of tension will be equal to the centripetal force.

Use the given mass and velocity to solve for the radius.

Centripetal force can be found using the equation:

In this situation, the radius is the length of the string. We are given the linear velocity and mass, as well as the radius, allowing us to solve for the centripetal force.

For this problem, we use the centripetal force equation:

We are given the mass, radius or rotation, and the linear velocity. Using these values, we can find the centripetal force.

This problem requires us to add torques about the pivot point. In order for the seesaw to be balanced, the torque must be equal on each side of the pivot point.

Use the equation for torque in this equation.

The force of each object will be equal to the force of gravity.

Gravity can be canceled from each side of the equation. for simplicity.

Now we can use the mass of the rock and the mass of the child. The total length of the seesaw is two meters, and the child sits at one end. The child's distance from the center of the seesaw will be one meter.

Solve for the distance between the rock and the center of the seesaw.

The metal bar is in rotational equilibrium, meaning there is no net torque. Use the wall pivot as the rotation point to eliminate having to calculate torque due to the unknown wall force, since the wall exerts no torque around the pivot. This leaves the rope tension and the weight of the bar as the only torque generators.

 Calculate the torques of those forces around the wall pivot with a standard procedure:

1)  Draw in the force vector arrows on the beam at their points of application.

2)  Draw a line through the force arrows extending to the edges of the drawing. This is the “line of force.”

3)  Draw a line perpendicular to the line of force from the axis of rotation (the wall pivot, in this case) to the line of force at the point where it is nearest the axis of rotation. This is the “perpendicular lever arm.”

The torque is then the force applied times its perpendicular lever arm around the axis of rotation.

Consider, for a uniform bar, the weight being applied at the center. The closest approach of the weight’s line of force to the pivot point is the center of the bar; hence, half the bar’s length is the perpendicular lever arm. So the torque of the weight, , around the pivot point is:

The tension is applied at the end of the bar, at a  angle with respect to the bar. The perpendicular lever arm can be calculated trigonometrically:

We can then find the torque generated by the tension force of the cable:

These torques produce rotations in the opposite direction, which is why they can cancel out to cause static equilibrium. Using the convention that counterclockwise rotations (as viewed in the diagram, with the wall on the left) are positive, the case of static equilibrium gives:

For this configuration, the tension in the cable happens to equal the weight of the bar.