Physics 110
Prelab 9

Introduction
{
Refer to sections 10.5 to 10.7  and 12.2 to 12.3 in Giancoli for this lab.}

Rotational equilibrium.
A net torque acts to cause an angular acceleration (changing rate of rotation) about some axis of rotation.  The magnitude of a torque is given by
                                                                                   

where R is the radial distance from the axis of rotation to the point of the force’s application, F is the magnitude of the force and  is the angle between the two.  It should be clear that the maximum torque will occur when a given force F is applied perpendicularly to the radial arm R (i.e. tangentially).


This explains why it’s easier to open a door when you push farther from the side with the hinges: for the same applied force you get a larger torque.
Just as many forces can act on an object at rest yielding a net force is zero and thus no translation, so may many torques act on an object at rest yielding a net torque of zero and no rotation.

fig 1

Consider the rod above of length L being supported horizontally by two strings, one at its right end and one a distance x from the right end.  Including gravity, there will be three forces on the rod. Note that the force of gravity can be thought of as acting at the center of the rod.  These forces will also create torques on the rod which will try to rotate it. 

Torque is a vector, it has magnitude and direction.  If a torque tries to induce a clockwise rotation about a given axis, the direction of that torque is away from you (we’ll call it negative).  The torque is pointed toward you and will be positive if it tries to induce a counterclockwise rotation. For a body to be in equilibrium the sum of the forces must be zero and the sum of the positive and negative torques must also be zero.

In the first experiment this week you will determine what forces FL and FR must be applied so that a suspended rod is in equilibrium.

PL1.  Explain why we should see FL + FR = Mg, where M is the mass of the suspended rod.

PL2.  In a static equilibrium problem, it is possible to choose any axis of rotation that you would like.  When calculating the torques on an object, it is often convenient to choose an axis of rotation at the location of one of the applied forces so that no torque will result from that force.  Choose the right end of the rod as the axis of rotation.  Calculate the sum of the torques with the right end of the rod as the axis of rotation. If x is the distance from the right end to FL and L is the length of the rod, show that FL = (MgL/2x).

PL3.  Suppose the length of the rod is 1 meter and its mass is 1 kg.  Using the midpoint of the rod as your axis of rotation, determine the force FR at the right end of the rod and the force FL  at x = 0.75 meters required for static equilibrium. 

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