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Fundamentals of Biomechanics

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inverse dynamics. Other scientists build<br />

complex computer models <strong>of</strong> biomechanical<br />

systems and use direct dynamics, essentially<br />

calculating the motion from the<br />

“what-if” kinetics and body configurations<br />

they input.<br />

Newton's Third Law<br />

Newton's third law <strong>of</strong> motion is called the<br />

Law <strong>of</strong> Reaction, because it is most <strong>of</strong>ten<br />

translated as: for every action there is an<br />

equal and opposite reaction. For every force<br />

exerted, there is an equal and opposite force<br />

being exerted. If a patient exerts a sideways<br />

force <strong>of</strong> +150 N on an elastic cord, there has<br />

to be –150-N reaction force <strong>of</strong> the cord on<br />

the patient's hand (Figure 6.4). The key insight<br />

that people <strong>of</strong>ten miss is that a force is<br />

really a mutual interaction between two<br />

bodies. It may seem strange that if you<br />

push horizontally against a wall, the wall is<br />

simultaneously pushing back toward you,<br />

but it is. This is not to say that a force on a<br />

free-body diagram should be represented<br />

by two vectors, but a person must understand<br />

that the effect <strong>of</strong> a force is not just on<br />

CHAPTER 6: LINEAR KINETICS 137<br />

Figure 6.3. Friction forces acting on ice skaters during push-<strong>of</strong>f and gliding. Newton' Second Law <strong>of</strong> Motion applied<br />

in the horizontal direction (see text) will determine the horizontal acceleration <strong>of</strong> the skater.<br />

one object. A free body diagram is one object<br />

or mechanical system and the forces<br />

acting on it, so the double vectors in<br />

Figures 6.4 and 6.5 can sometimes be confusing<br />

because they are illustrating both<br />

objects and are not true free body diagrams.<br />

If someone ever did not seem to kiss<br />

you back, you can always take some comfort<br />

in the fact that at least in mechanical<br />

terms they did.<br />

An important implication <strong>of</strong> the law <strong>of</strong><br />

reaction is how reaction forces can change<br />

the direction <strong>of</strong> motion opposite to our applied<br />

force when we exert our force on objects<br />

with higher force or inertia (Figure<br />

6.5a). During push-<strong>of</strong>f in running the athlete<br />

exerts downward and backward push<br />

with the foot, which creates a ground reaction<br />

force to propel the body upward and<br />

forward. The extreme mass <strong>of</strong> the earth easily<br />

overcomes our inertia, and the ground<br />

reaction force accelerates our body in the<br />

opposite direction <strong>of</strong> force applied to the<br />

ground. Another example would be eccentric<br />

muscle actions where we use our muscles<br />

as brakes, pushing in the opposite direction<br />

to another force. The force exerted

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