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We need to evaluate
I=∫−ππ1+cos2y2y(1+siny)dy.
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Split the integrand:
1+cos2y2y(1+siny)=1+cos2y2y+1+cos2y2ysiny.
So,
I=∫−ππ1+cos2y2ydy+∫−ππ1+cos2y2ysinydy.
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Use parity (odd/even properties):
- y is odd.
- cos2y is even, so 1+cos2y is even.
- Hence 1+cos2y2y is odd.
Therefore,
∫−ππ1+cos2y2ydy=0.
- Now consider
1+cos2y2ysiny.
Here:
- y is odd,
- siny is odd,
- product ysiny is even,
- denominator 1+cos2y is even.
So the whole function is even.
Thus,
I=∫−ππ1+cos2y2ysinydy=2∫0π1+cos2y2ysinydy=4∫0π1+cos2yysinydy.
- Let
J=∫0π1+cos2yysinydy.
Use integration by parts:
- Take u=y⇒du=dy,
- Take dv=1+cos2ysinydy.
Now compute v:
Let t=cosy, then dt=−sinydy.
So,
∫1+cos2ysinydy=−∫1+t2dt=−tan−1(t)=−tan−1(cosy).
Hence,
v=−tan−1(cosy).
Therefore,
J=[−ytan−1(cosy)]0π+∫0πtan−1(cosy)dy.
- Evaluate the boundary term:
- At y=π, cosπ=−1, so tan−1(−1)=−4π.
Thus,
−πtan−1(cosπ)=−π(−4π)=4π2.
- At y=0, the term is 0.
So,
J=4π2+∫0πtan−1(cosy)dy.
- Now evaluate
K=∫0πtan−1(cosy)dy.
Use the substitution y↦π−y:
∫0πtan−1(−cosy)dy.
Since tan−1(−x)=−tan−1(x),
K=−∫0πtan−1(cosy)dy=−K.
Hence,
K=0.
Therefore,
J=4π2.
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Finally,
I=4J=4⋅4π2=π2.
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So the correct option is
π2
which is option B.