Problem:
Solution:
We will skip part (a) because it is basically the same as this previous exercise. The solution is (t−sint,1−cost)
For part (b), we compute the arc length as
2π∫0|α′(t)|dt=2π∫0√α′(t)⋅α′(t)dt=2π∫0√(1−cost)2+sin2tdt=2π∫0√1−2cost+cos2t+sin2tdt=2π∫0√2−2costdt
The rest is really just an integration problem, let x=cost, so
dx=−sintdt=−√1−cos2tdt=−√1−x2dtdt=dx−√1−x2
When t=0, x=cos0=1
When t=π, x=cosπ=0
2π∫0√2−2costdt=2π∫0√2−2costdt=2−1∫1√2−2xdx−√1−x2=21∫−1√2−2x1−x2dx=2√21∫−1√11+xdx=4√2√1+x|1−1=8
Just as an aside, I used numerical integration and arc length approximation to make sure the answer is correct.
Solution:
We will skip part (a) because it is basically the same as this previous exercise. The solution is (t−sint,1−cost)
For part (b), we compute the arc length as
2π∫0|α′(t)|dt=2π∫0√α′(t)⋅α′(t)dt=2π∫0√(1−cost)2+sin2tdt=2π∫0√1−2cost+cos2t+sin2tdt=2π∫0√2−2costdt
The rest is really just an integration problem, let x=cost, so
dx=−sintdt=−√1−cos2tdt=−√1−x2dtdt=dx−√1−x2
When t=0, x=cos0=1
When t=π, x=cosπ=0
2π∫0√2−2costdt=2π∫0√2−2costdt=2−1∫1√2−2xdx−√1−x2=21∫−1√2−2x1−x2dx=2√21∫−1√11+xdx=4√2√1+x|1−1=8
Just as an aside, I used numerical integration and arc length approximation to make sure the answer is correct.
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