Forces in Equilibrium
If an object is neither moving through space (translating) nor rotating, 
it is said to be in static equilibrium. The sum of the external forces acting 
on the object must be zero (recall forces add as vectors); and similarly 
the sum of the external torques must be zero.   
The forces in this lab will be tensions and weights.  The magnitude of the weights 
will be determined by using known masses and using the formula mg. Furthermore, 
the direction of weight is known to be vertically down. Because the masses are in static 
equilibrium, we will be able to determine (most of) the tensions.  Next, we will 
use pulleys to change the directions of the tensions.  The new direction of the tensions 
will be observable since tensions act along the string.  Using a protractor 
to measure angles (directions), we can apply the ideas of vector addition, i.e. choosing 
a coordinate system, breaking forces into components in that coordinate system, 
and adding the components, to test our notion of equilibrium and then to use it 
to determine unknown forces.    
A Force Sensor (a type of spring balance) can be used to measure forces. In the 
third part of the lab, we test a Force Sensor using known weights. In the last part 
of the lab we will use the pulley as a simple machine. 
 
Part 1: Confirming equilibrium
- Using ringstands, pulleys, strings and hangers, set up 
apparatus as shown below 
 
 
 
 
- Later we will need the middle string to establish the vertical 
direction, so there should be few centimeters between the knot 
and the hanger.  
- Place masses on the hangers. All three should have 
  different masses. Provided none of the masses is too large, the middle mass 
  will move horizontally and vertically until it finds a position of stable 
  equilibrium. Record the masses (include the mass of the hanger) and enter the 
corresponding tensions in the table below. 
    
 
 
| m1 (   )
 | m2 (   )
 | m3 (   )
 | T1 (   )
 | T2 (   )
 | T3 (   )
 | q1 (   )
 | q2 (   )
 |  |  |  |  |  |  |  |  |  |  
 
 
 
- Use a protractor to measure the angles between the 
  strings and the vertical. As shown below you can use the the string attached 
  to middle hanger to establish a vertical line.
 
 
- The knot must be in equilibrium, that is, the net 
  force on it must be zero. Therefore the horizontal components must be zero 
  (within experimental error), and similarly the vertical components must be 
  zero. Confirm that these conditions are met.
 
Part 2: Using equilibrium to find unknowns
- Tie another string (a few centimeters in length) and attach a 
fourth mass to the arrangement as shown below. The mass does 
not have to be a hanger. (Try to make sure none of the angles is close 
to 0 or 90 degrees.) 
 
 
- Record the masses, tensions and angles.
 
 
| m1 (   )
 | m2 (   )
 | m3 (   )
 | m4 (   )
 | T1 (   )
 | T2 (   )
 | T3 (   )
 | T4 (   )
 | q1 (   )
 | q2 (   )
 | q3 (   )
 | q4 (   )
 |  |  |  |  |  |  |  |  |  |  |  |  |  |  
 
 
 
- The tension along the string between knots A and B is unknown.  There are four distinct equilibrium 
conditions, each of which should allow you to calculate the 
magnitude of the unknown tension 
 
 
- the x components for the knot A tensions 
- the y components for the knot A tensions 
- the x components for the knot B tensions 
- the y components for the knot B tensions
 
 
- Find the magnitude of the unknown tension using each condition. Show your
        work!
  Calculate the percent difference (relative difference) between each value and 
  the average. Did you obtain the same results within an acceptable amount of 
  experimental error? 
 
 
| Method | Unknown Tension | Percent Difference
 |  | 1 |  |  |  | 2 |  |  |  | 3 |  |  |  | 4 |  |  |  | Ave |  |  |  
 
 
 
 
- Imagine you had neglected to calculate 
q4, 
  use the equilibrium conditions to calculate it. Compare the value you find 
  with the measured value. Is the difference between your measured and 
  calculated value acceptably small?
		Part 3. Calibrating the Force Sensor.
		
			- 
				Attach a force sensor to a ringstand as shown below.
				
 
 
 
 
- 
			    Plug the Force Sensor into Analog Channel A. Bring up Data Studio, click on the 
			icon for Analog Channel A icon, and choose Force Sensor 
			from the menu.
- 
				BEFORE
			hanging a hanger from the Force Sensor, press the TARE button on the side of 
			it. This step is supposed to establish the "zero" of the Force Sensor.
- 
			Hang the hanger from the force sensor. Add a mass of 100 g.
- 
			Press Start and take force data for a few seconds.
- 
			Table the data and press the SIGMA button to obtain the mean force. We are only 
			interested in getting the magnitude of the force (which is necessarily 
			positive) from the source, so you don't have to worry about the negative sign 
			the force sensor gives.
- 
				Repeat the measurements with 200 g and 300g on the hanger.
				
		
			
				| Mass (kg) | Force (N) (Measured)
 | Force (N) (Theory, mg)
 |  
				| 0.150 |  |  |  
				| 0.250 |  |  |  
				| 0.350 |  |  |  
 
 
Do you observe any errors in your force sensor readings? If so, are they 
			systematic or random? Explain.
Part 4 Pulley Effect
		
Arrange your apparatus based on the figure below. When W1 (hanger and 
added mass) has a mass of 100g what is the sensor's reading? Repeat with 
150g, 200g and 250g. What is the sensor holding up? With the 250g attached 
slowly pull the force sensor 4cm. By how much does W1 move?

	| Mass (kg) | Force (N) | 
	| 0.100 |  | 
	| 0.150 |  | 
	| 0.200 |  | 
	| 0.250 |  |