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College Trigonometry, 2011a

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11.5 Graphs of Polar Equations 947<br />

Again, we invite the reader to show that plotting the curve for values of θ outside [0, 2π]<br />

results in retracing a portion of the curve already traced. Our final graph is below.<br />

6<br />

r<br />

y<br />

4<br />

θ = 2π 3<br />

2<br />

2<br />

2π<br />

3<br />

π<br />

2<br />

π<br />

4π<br />

3<br />

3π<br />

2<br />

2π<br />

θ<br />

θ = 4π 3 −2<br />

2 6<br />

x<br />

−2<br />

r = 2 + 4 cos(θ) intheθr-plane<br />

r = 2 + 4 cos(θ) inthexy-plane<br />

3. As usual, we start by graphing a fundamental cycle of r =5sin(2θ) intheθr-plane, which in<br />

this case, occurs as θ ranges from 0 to π. We partition our interval into subintervals to help<br />

us with the graphing, namely [ 0, π ] [<br />

4 , π<br />

4 , π ] [<br />

2 , π<br />

2 , 3π ] [<br />

4 and 3π<br />

4 ,π] .Asθ ranges from 0 to π 4 , r<br />

increases from 0 to 5. This means that the graph of r =5sin(2θ) inthexy-plane starts at<br />

the origin and gradually sweeps out so it is 5 units away from the origin on the line θ = π 4 .<br />

5<br />

r<br />

y<br />

π<br />

4<br />

π<br />

2<br />

3π<br />

4<br />

π<br />

θ<br />

x<br />

−5<br />

Next, we see that r decreases from 5 to 0 as θ runs through [ π<br />

4 , π ]<br />

2 , and furthermore, r is<br />

heading negative as θ crosses π 2 . Hence, we draw the curve hugging the line θ = π 2<br />

(the y-axis)<br />

as the curve heads to the origin.

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