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College Trigonometry, 2011a

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732 Foundations of <strong>Trigonometry</strong><br />

Theorem 10.3 gives us what we need to describe the position of an object traveling in a circular<br />

path of radius r with constant angular velocity ω. Suppose that at time t, the object has swept<br />

out an angle measuring θ radians. If we assume that the object is at the point (r, 0) when t =0,<br />

the angle θ is in standard position. By definition, ω = θ t<br />

which we rewrite as θ = ωt. According<br />

to Theorem 10.3, the location of the object Q(x, y) on the circle is found using the equations<br />

x = r cos(θ) =r cos(ωt) andy = r sin(θ) =r sin(ωt). Hence, at time t, the object is at the point<br />

(r cos(ωt),rsin(ωt)). We have just argued the following.<br />

Equation 10.3. Suppose an object is traveling in a circular path of radius r centered at the<br />

origin with constant angular velocity ω. Ift = 0 corresponds to the point (r, 0), then the x and<br />

y coordinates of the object are functions of t and are given by x = r cos(ωt) andy = r sin(ωt).<br />

Here, ω>0 indicates a counter-clockwise direction and ω

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