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Fundamentals of Biomechanics

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156 FUNDAMENTALS OF BIOMECHANICS<br />

Figure 6.18. The mechanical work done on a weight in this rowing exercise is the product <strong>of</strong> the force and the<br />

displacement.<br />

load is constant over the duration <strong>of</strong> the<br />

movement. Calculus is necessary to calculate<br />

the work <strong>of</strong> the true time-varying<br />

forces applied to weights in exercises. This<br />

example also assumes that the energy losses<br />

in the pulleys are negligible as they<br />

change the direction <strong>of</strong> the force created by<br />

the patient.<br />

Note that mechanical work can only be<br />

done on an object when it is moved relative<br />

to the line <strong>of</strong> action <strong>of</strong> the force. A more<br />

complete algebraic definition <strong>of</strong> mechanical<br />

work in the horizontal (x) direction that<br />

takes into account the component <strong>of</strong> motion<br />

in the direction <strong>of</strong> the force on an object<br />

would be W = (F cos ) • d x . For example, a<br />

person pulling a load horizontally on a dolly<br />

given the data in Figure 6.19 would do<br />

435 Nm or Joules <strong>of</strong> work. Only the horizontal<br />

component <strong>of</strong> the force times the displacement<br />

<strong>of</strong> object determines the work<br />

done. Note also that the angle <strong>of</strong> pull in this<br />

example is like the muscle angle <strong>of</strong> pull analyzed<br />

earlier. The smaller the angle <strong>of</strong> pull,<br />

the greater the horizontal component <strong>of</strong> the<br />

force that does work to move the load.<br />

The vertical component <strong>of</strong> pull does<br />

not do any mechanical work, although it<br />

may decrease the weight <strong>of</strong> the dolly or<br />

load and, thereby decrease the rolling friction<br />

to be overcome. What is the best angle<br />

to pull in this situation depends on many<br />

factors. Factoring in rolling friction and the<br />

strength (force) ability in various pulling<br />

postures might indicate that a higher angle<br />

<strong>of</strong> pull that doesn't maximize the horizontal<br />

force component may be “biomechanically”<br />

effective for this person. The inertia <strong>of</strong><br />

the load, the friction under the person's<br />

feet, and the biomechanical factors <strong>of</strong><br />

pulling from different postures all interact<br />

to determine the optimal angle for pulling<br />

an object. In fact, in some closed kinematic<br />

chain movements (like cycling) the optimal<br />

direction <strong>of</strong> force application does not always<br />

maximize the effectiveness or the<br />

component <strong>of</strong> force in the direction <strong>of</strong> motion<br />

(Doorenbosch et al., 1997).<br />

Mechanical work does not directly correspond<br />

to people's sense <strong>of</strong> muscular effort.<br />

Isometric actions, while taking considerable<br />

effort, do not perform mechanical

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