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letamp;#39;s look at an example free body diagram first letamp;#39;s draw an example diagram here we have a mass M1 has a couple of forces acting on it and weamp;#39;ve also indicated our direction of motion as X1 with the zero point of X1 being this bar at the bottom so as we pull with forces FS2 and F3 that goes in the direction of X1 and force F1 is opposite the direction of forces FS2 and F3 so using the fals ma the traditional and probably by now very familiar Newtonian laws of translational motion now we can actually write fub1 FS2 and F3 as forces on the left hand side and the mass times acceleration is the right hand side so again we changed the sign of F1 to indicate that itamp;#39;s traveling in the opposite direction that X1 indicates we can also change as you see here the direction of F3 itamp;#39;s plus if F3 is pointing up and then itamp;#39;s minus IS F 3 is pointing down so as we change that direction we change the sign of F3 on the right hand side likewise we can
