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Straight line connects midpoint of joints on either end |
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Angle between line of pull and mechanical axis of bone |
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changes angle of pull increases rotary component patella |
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Act at the same point of application But at different angles |
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Not in the same line But parallel to eachother |
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a force whose direction is not in line with the center of gravity of a freely moving object or the center of rotation of an object with a fixed axis of rotation. |
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Turning effect of eccentric force Product of force magnitude and length of moment arm. |
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Perpendicular to line of force Distance to axis of rotation |
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Change moment arm or force |
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Muscle force vectors for torque |
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Rotary component produces torque Stabilizing component acts along mechanical axis of bone |
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Summation of torques results in... |
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Either: no motion, linear motion, or rotary motion |
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Sum of torques Clockwise are negative Counterclockwise are positive |
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A rigid bar that can rotate about a fixed point when a force is applied to overcome a resistance |
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Balance 2 or more forces Favor force production Favor speed and range of motion Change the direction of the applied force |
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Bones = levers Joint = fulcrum Muscle = force |
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Fulcrum Point of resistance Point of force applied |
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Perpendicular distance between fulcrum and line of force of effort |
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Perpendicular distance between fulcrum and line of resistance force |
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Effort -> fulcrum -> resistance |
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Fulcrum -> resistance -> effort |
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Fulcrum -> effort -> resistance |
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Acceleration of rotating bodies |
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Torque = moment of inertia X angular acceleration |
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Depends on:
Quantity of rotating mass
Distribution around axis of rotation
I = Σmr2, m = mass, r = perpendicular distance between mass and axis of rotation |
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Body position affects mass distribution and therefore inertia |
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Tendency to persist in rotary motion
Product of moment of inertia and angular velocity |
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