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College Trigonometry, 2011a

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942 Applications of <strong>Trigonometry</strong><br />

[ ]<br />

0,<br />

π<br />

2 , we have that the curve begins to retrace itself at this point. Proceeding further, we find<br />

that when 3π 2<br />

≤ θ ≤ 2π, we retrace the portion of the curve in Quadrant IV that we first traced<br />

out as π 2<br />

≤ θ ≤ π. The reader is invited to verify that plotting any range of θ outside the interval<br />

[0,π] results in retracting some portion of the curve. 4 We present the final graph below.<br />

6<br />

r<br />

y<br />

3<br />

3<br />

π<br />

2<br />

π<br />

θ<br />

3 6<br />

x<br />

−3<br />

−3<br />

−6<br />

r =6cos(θ) intheθr-plane<br />

r = 6 cos(θ) inthexy-plane<br />

Example 11.5.2. Graph the following polar equations.<br />

1. r =4− 2sin(θ) 2. r = 2 + 4 cos(θ) 3. r =5sin(2θ) 4. r 2 =16cos(2θ)<br />

Solution.<br />

1. We first plot the fundamental cycle of r =4− 2sin(θ) ontheθr-axes. To help us visualize<br />

what is going on graphically, we divide up [0, 2π] into the usual four subintervals [ 0, π ] [<br />

2 , π<br />

[ ] [ 2 ,π] ,<br />

π,<br />

3π<br />

2 and 3π<br />

2 , 2π] , and proceed as we did above. As θ ranges from 0 to π 2<br />

, r decreases from<br />

4 to 2. This means that the curve in the xy-plane starts 4 units from the origin on the positive<br />

x-axis and gradually pulls in towards the origin as it moves towards the positive y-axis.<br />

r<br />

y<br />

6<br />

θ runs from 0 to π 2<br />

4<br />

x<br />

2<br />

π<br />

2<br />

π<br />

3π<br />

2<br />

2π<br />

θ<br />

4 The graph of r =6cos(θ) looks suspiciously like a circle, for good reason. See number 1a in Example 11.4.3.

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