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Fundamentals of Biomechanics

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outs. We will see in the next section that<br />

muscle mechanical properties also change<br />

in response to activity and inactivity.<br />

THREE MECHANICAL CHARAC-<br />

TERISTICS OF MUSCLE<br />

Previously we discussed the passive tension<br />

in an MTU as it is passively stretched.<br />

Now it is time to examine the tensile forces<br />

the MTU experiences in the wide variety<br />

actions, lengths, and other active conditions<br />

encountered in movement. The force potential<br />

<strong>of</strong> an MTU varies and can be described<br />

by three mechanical characteristics. These<br />

characteristics deal with the variations in<br />

muscle force because <strong>of</strong> differences in velocity,<br />

length, and the time relative to activation.<br />

Force–Velocity Relationship<br />

The Force–Velocity Relationship explains<br />

how the force <strong>of</strong> fully activated muscle<br />

varies with velocity. This may be the most<br />

important mechanical characteristic since<br />

all three muscle actions (eccentric, isometric,<br />

concentric) are reflected in the graph.<br />

CHAPTER 4: MECHANICS OF THE MUSCULOSKELETAL SYSTEM 79<br />

We will see that the force or tension a muscle<br />

can create is quite different across actions<br />

and across the many speeds <strong>of</strong> movement.<br />

The discovery and formula describing<br />

this fundamental relationship in concentric<br />

conditions is also attributed to A. V.<br />

Hill. Hill made careful measurements <strong>of</strong><br />

the velocity <strong>of</strong> shortening when a preparation<br />

<strong>of</strong> maximally stimulated frog muscle<br />

was released from isometric conditions.<br />

These studies <strong>of</strong> isolated preparations <strong>of</strong><br />

muscle are performed in what we term in<br />

vitro (Latin for “in glass”) conditions.<br />

Figure 4.7 illustrates the shape <strong>of</strong> the complete<br />

Force–Velocity Relationship <strong>of</strong> skeletal<br />

muscle. The Force–Velocity curve essentially<br />

states that the force the muscle can<br />

create decreases with increasing velocity <strong>of</strong><br />

shortening (concentric actions), while the<br />

force the muscle can resist increases with<br />

increasing velocity <strong>of</strong> lengthening (eccentric<br />

actions). The force in isometric conditions<br />

is labeled P 0 in Hill's equation. The<br />

right side <strong>of</strong> the graph corresponds to how<br />

the tension potential <strong>of</strong> the muscle rapidly<br />

decreases with increases in speed <strong>of</strong> concentric<br />

shortening. Also note, however, that<br />

Figure 4.7. The in vitro Force–Velocity Relationship <strong>of</strong> muscle. Muscle force potential rapidly decreases with increasing<br />

velocity <strong>of</strong> shortening (concentric action), while the force within the muscle increases with increasing velocity<br />

<strong>of</strong> lengthening (eccentric action). The rise in force for eccentric actions is much higher than illustrated.

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