Unlike the force table shown, we conducted this experiment without using the pulleys. Instead, we directly hung the strings on the edge of the circular platform. As stated in the procedure, we first designated two masses for the first two vectors then computed their vertical and horizontal components to be used in determining the magnitude and direction of the equilibrant represented by R in the laboratory report. Then, we positioned the third vector based on the computed mass and angle for the equilibrant. We did minor adjustments to position the middle ring exactly in the center and noted these adjustments to be compared on the computed values. In order to compute the vertical and horizontal components of each of the vectors, I used y = msinθ and x = mcosθ, respectively, where m is the displacement and θ is the direction or angle of the vector. To determine the magnitude of the resultant force, use the formula R = √(x2 + y2), where x and y are the summations of the x's and y's of the previously computed horizontal and vertical component. Furthermore, to compute the direction of the resultant, use tan θ = y/x. Note that it is not the resultant force but the equilibrant force that will balance the system. Henceforth, the direction to be used should be opposite to that of resultant force.