Sunday 26 June 2016

experiment 03: FORCES OF EQUILIBRIUM


Experimental set-up:

You are going to study the various forces acting on a body in equilibrium. As you know from

lectures (or will find out in the near future), a body is in equilibrium (i.e. not accelerating)

when the sum of all the forces acting on it are equal to zero. In this experiment you are going

to study an object with 3 and 4 forces acting on it, and show that the vector sum of those

forces is zero, using both the polygon and component methods (discussed in the analysis

section below). The apparatus you will use will consist of a drawing board and a number of

pulleys on a frame, masses, some twine and an object (in this case a small ring).

.
Figure 6a. Schematic diagram of apparatus Figure 6b. Vector diagram of forces on object


When you initially put the apparatus together and put the masses on the twine, the ring will

move slightly and then come to rest in an equilibrium position. When the ring in at rest, i.e. in

equilibrium, the total force acting on it is zero.
The gravitational force (or weight) exerted on each mass is mg (where g is the acceleration due

to gravity ~ 9.81 m/s2). In figure 6a above there are 3 masses (m1, m2 & m3), and each exerts a

force on the object of size m1g, m2g & m3g, with the forces acting along the direction of the


string connecting the mass to the object. The forces acting on the ring then look like those in

figure 6b.

By taping a piece of graph paper on the drawing board behind the twine and marking the

position of the three pieces of string (by marking 2 points for each piece, one close to the

object and another close to the pulley), and then drawing vectors along these directions with
lengths proportional to the masses (e.g. 1 cm 100 g) you will have made a vector diagram of


the forces on the object.

You can then use the polygon method or the method of components (discussed in the analysis

section below) to show that the vector sum of these forces is zero.
 

 


Procedure:

1. Preparation:

Tape a sheet of graph paper onto the face of the board.

Tie three pieces of thread to the ring and pass two of them over the upper pulleys


leaving the third to hang free. Tie a loop at the end of each piece of thread and suspend

a mass hanger from each loop.
2. Starting up:

Load each mass hanger with masses but keep the ring fairly central on the board.

With a pencil, mark on the paper the position of each piece of thread by taking a point


at either end.
Note the masses (m1, m2 & m3) suspended from each thread.

Remove the graph paper and draw vectors in the direction of the strings, with lengths


directly proportional to the appropriate masses.
3. Making measurements:

Vary M1, M2 and M3 and repeat this procedure for another different equilibrium


situation.
Using the third pulley, follow the above procedure with 4 masses.



Note: Each person must submit his or her own set of 4 original vector diagrams on

graph paper, stapled to the answer sheet (part A4 of answer sheet).

4. Data presentation:

For the first vector diagram you obtained, with 3 masses, use the polygon method to


draw the resultant vector (on the same sheet of graph paper). Measure the length of the

resultant vector
For the second vector diagram you obtained, again with 3 masses, calculate the x- and ycomponents

of each vector  and the x- and y-components of


the resultant vector.
For the third vector diagram you obtained, this time with 4 masses, once again use the


polygon method to draw the resultant vector (on the same sheet of graph paper).

Measure the length of the resultant vector
For the fourth vector diagram you obtained, again with 4 masses, calculate the x- and ycomponents

of each vector ) and the x- and y- components of


the resultant vector.
Analysis:

Diagrammatic representation of vectors:

The directional nature of vectors means that a single number cannot describe them. An arrow

is generally used to represent vectors diagrammatically. The length of the arrow is

proportional to the vector magnitude, while the direction is parallel to the vector direction.

This method of representing vectors also allows us to very easily see how vectors add.
The vector A may be represented on a diagram by drawing an arrow the length of which is


proportional to the magnitude of the vector quantity. The arrow is drawn in the direction of
 

the vector.


Adding vectors:

The resultant of a number of vectors is the single vector which would have the same effect as
all the original vectors together. R = A + B + C means that R is the resultant of the vectors A,

B and C. We can visualise how vectors are added in a geometric manner. We can actually


perform the addition in two ways, either using a mainly geometrical methods (polygon
method) or a more arithmetically based method (component method). The two methods



produce the exact same results.

Polygon Method;

The resultant of two or more vectors may be obtained by drawing them "head-to-tail" (in any

order). The line drawn to complete the triangle or polygon represents the resultant, which is

pointed from the tail of the first vector to the arrow-head of the last vector.