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Fundamentals of Biomechanics

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144 FUNDAMENTALS OF BIOMECHANICS<br />

Figure 6.9. Right-angle trigonometry is used to find the components <strong>of</strong> a vector like the iliopsoas muscle force illustrated.<br />

Notice the muscle force is resolved into components along the longitudinal axis <strong>of</strong> the femur and at right<br />

angles to the femur. The right angle component is the force that creates rotation (F R ).<br />

understand where the largest changes occur<br />

and what angles <strong>of</strong> force application are<br />

best. Let's look at a horizontal component<br />

<strong>of</strong> a force in two dimensions. This is analogous<br />

to our iliopsoas example, or how any<br />

force applied to an object will favor the horizontal<br />

over the vertical component. A cosine<br />

function is not a linear function like<br />

our spring example in chapter 2. Figure 6.10<br />

plots the size <strong>of</strong> the cosine function as a percentage<br />

<strong>of</strong> the resultant for angles <strong>of</strong> pull<br />

from 0 to 90º.<br />

A 0º (horizontal) angle <strong>of</strong> pull has no<br />

vertical component, so all the force is in the<br />

horizontal direction. Note that, as the angle<br />

<strong>of</strong> pull begins to rise (0 to 30º), the cosine or<br />

horizontal component drops very slowly,<br />

so most <strong>of</strong> the resultant force is directed<br />

horizontally. Now the cosine function begins<br />

to change more rapidly, and from 30 to<br />

60º the horizontal component has dropped<br />

from 87 to 50% the size <strong>of</strong> the resultant<br />

force. For angles <strong>of</strong> pull greater than 60º, the<br />

cosine drops <strong>of</strong>f very fast, so there is a dra-

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