To solve this, we must employ a structural transformation. We define the substitution:
cscx+cotx=eu
Substituting our original definition, we obtain:
−cscx(eu)dx=eudu
The
eu terms cancel out, leading to the elegant differential relation:
cscxdx=−du
To express
2cscx in terms of
u, we use the identity
csc2x−cot2x=1. Factoring this as a difference of squares, we have:
(cscx−cotx)(cscx+cotx)=1
Since
cscx+cotx=eu, it follows that
cscx−cotx=e−u. Adding these two equations eliminates the cotangent terms:
2cscx=eu+e−u
We rewrite the integrand as
(2cscx)16⋅(2cscx). Substituting our exponential expressions, we get:
(eu+e−u)16⋅2⋅(−du)
Next, we transform the limits of integration. At the lower limit
x=π/4:
eu=csc(π/4)+cot(π/4)=2+1⇒u=ln(1+2) At the upper limit
x=π/2:
eu=csc(π/2)+cot(π/2)=1+0=1⇒u=0
By flipping the limits to absorb the negative sign, we arrive at the final, simplified form:
I=∫0ln(1+2)2(eu+e−u)16du This result demonstrates the power of calculus in distilling chaotic trigonometric expressions into clean, solvable exponential forms.