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Every point in a body rotating about a fixed axis moves in a circle whose center is on the axis has a radius, r. Any point on the radius will sweep out the same angle in the same time. One radian, rad, is defined as the angle subtended by an arc whose length is equal to the radius. In the drawing to the left, the length, l, is equal to the radius, r. = 1 rad.
l 360o = 2rad
Omega, , is the average when measured over long periods of time and instantaneous when the time approaches zero. Units are rad/s. As shown in the drawing to the left, the instantaneous velocity is larger as you move farther from the axis, but , is constant. Thus the is independent of the radius.
is the average angular acceleration when measured over long periods of time and instantaneous when the time approaches zero. There is a simple relationship between Angular and Linear measurements. x = r aT = r
a = aT + aC Remember that aT and aC are perpendicular to each other. In the section on circular motion, we related centripetal
acceleration to the linear velocity and radius. We can also relate them to
angular velocity. v2
( r
)2 At times we relate the angular velocity to the frequency of rotation, f. The frequency is the number of complete rotations in one seconds. One revolution is equal to an angular displacement of 2rad.
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