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Factors Influencing Movement
1. Magnitude of net Torque 2. Inertial characteristics of object such as it’s rotational inertia (I), friction factors 3. Pathway available
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Rotary Motion represented by a straight line
line starts at the axis of rotation line ends at a selected point on the body or segment being examined
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KINEMATICS Linear Rotary
v = d/t omega = ÷ t alpha = 2- 1 ÷ t a = v2 - v1 ÷ t d = vt theta = t
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: Angular Velocity How fast a rotating body/segment changes its position measured in radians or degrees per second radian = 57.3 degrees direction is either cw- or ccw+
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v of a Point on Rotating Body
important in throwing, kicking, striking r --> radius of rotation --> distance from axis to a selected point linear distance d = r linear velocity v = r
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Radius = from trunk longitudinal axis to fingers
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“Basic Biomechanics” 4th edition
FIG page 373 “Basic Biomechanics” 4th edition by Susan J. Hall
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Figure H.1 on page 315 is the same for points A, B, and C
A, B, C = 2 rads or degrees [57.3 x 2] is the same for points A, B, and C v is not the same for points A, B, and C A, B, C 4 rads per second r increases from A (0.3) to B (0.6) to C (0.9)
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: Angular Acceleration
rare in human motion to have constant most motion has continual = ÷ t = large change in in a short time = small change in over a long time
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Slow Pitcher Fast Pitcher
= 5 radians t = 0.2 seconds = ÷ t = 20 radians t = 0.2 seconds = ÷ t = 5 ÷ = 25 rads/sec/sec = 20 ÷ = 100 rads/sec/sec
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Average Instantaneous
examining the time it takes for a body, segment, or implement to complete a motion useful in qualitative analysis of motion examining the at a particular point in the ROM v = r determines the instantaneous v of any point on a system
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= T ÷ I (Newton’s 2nd Law)
Rotational Inertia : I Resistance to a change in (angular accel.) I = mr² OR I = mk² = T ÷ I (Newton’s 2nd Law) T = I
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Examples of I = mr² 1. arm swing with elbows extended/flexed
2. Figure H.3b on page as r doubles I quadruples 3. turntable demonstration
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r of Rotation r of Gyration
asymmetrical systems distance from the axis of rotation to a point where all the mass is concentrated I = mk² symmetrical systems distance from the axis of rotation to a precise point on a rotating system v = r
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