**Problem 1:**Calculate the net torque exerted by

*F*

_{1}= 30 N and

*F*

_{2}= 50 N in the figure below. You may assume that both forces act on a single rigid body.

Two forces acting on a single rigid body

We begin be calculating the magnitude of each torque individually. Recall that

*τ*=*Fr*sin*θ*. Thus*τ*_{1}= (30)(1)sin 120 = 26.0 N-m and*τ*_{2}= (50)(1)sin 30 = 25 N-m. As we can see from the figure,*τ*_{1}acts counterclockwise while*τ*_{2}acts clockwise. Thus the two torques act in opposite directions, and the net torque is thus 1 N-m in the counterclockwise direction.**Problem2 :**

Two cylinders of the same mass and shape, one hollow and one solid, are set on a incline and allowed to roll down. Which cylinder will reach the bottom of the incline first? Why?

Since both cylinders have the same shape, they will experience the same forces, and thus the same net torque. Recall that

*τ*=*Iα*. Thus the cylinder with the smaller moment of inertia will accelerate more quickly down the incline. Think of each cylinder as a collection of particles. The average radius of a particle in the solid cylinder is smaller than the hollow one, as most of the mass of the hollow one is concentrated at a larger radius. Since moment of inertia varies with*r*^{2}, it is clear that the solid cylinder will have a smaller moment of inertia, and thus a larger angular acceleration. The solid cylinder will reach the bottom of the incline first.**Problem3 :**

A simple pendulum of mass

*m*on a string of radius*r*is displaced from vertical by an angle*θ*, as shown below. What is the torque provided by gravity at that point?
A gravitational force acting on a simple pendulum

We begin by resolving the gravitational force into tangential and radial components, as shown below:

A gravitational force acting on a simple pendulum, shown resolved into components

*F*sin

*θ*=

*mg*sin

*θ*. This force acts at a distance

*r*from the axis of the rotation. Thus the magnitude of the torque is given by:

*τ*=

*Fr*= (

*mg*sin

*θ*)

*r*=

*mgr*sin

*θ*

**Problem4 :**

See the last problem. What is the angular acceleration of the pendulum at that point?

We already know the torque acting on the pendulum. Recall that

*τ*=*Iα*. Thus, to find the angular acceleration we need to compute the moment of inertia of the pendulum. Fortunately, it is simple in this case. We can treat the mass on the pendulum as a single particle of mass*m*and radius*r*. Thus*I*=*mr*^{2}. With this information we can solve for*α*:*α*= = =

**Problem5 :**

A revolving door is common in office buildings. What is the magnitude of the torque exerted on a revolving door of mass 100 kg if two people push on opposite sides of the door with a force of 50 N at a distance of 1 m from the axis of the door, as shown below? Also, the moment of inertia of a revolving door is given by

*I*= . Find the resultant angular acceleration assuming no resistance.
Two people pushing on a revolving door

Although it looks like the forces are directed in opposite directions, and thus cancel out, we must remember that we are working with angular motion here. In fact, both forces point in the counterclockwise direction, and can be considered to have the same magnitude and direction. In addition, they are both perpendicular to the radial direction of the door, so the magnitude of the torque by each one is given by:

*τ*=*Fr*= (50 N)(1 m) = 50 N-m. As we stated, the two forces act in the same direction, so the net torque is simply:*τ*= 100 N-m.
Next we have to calculate angular acceleration. We already know the net torque and thus must find the moment of inertia. We are given the formula

*I*= . We are given the mass, and from the figure we see that the radius is simply 1.5 m. Thus:*α*= = = rad/s

^{2}