The integral ∫0π/42tan3xdx simplifies to 1−log2 by rewriting tan3x=tanx(sec2x−1), splitting into two integrals, and using substitution u=tanx for the first part while the second part is a standard logarithmic integral.
Why This Approach Works
The integrand 2tan3x looks tricky because tan3x doesn't have a simple antiderivative directly. But here's the key insight: tan3x=tanx⋅tan2x, and tan2x=sec2x−1 (from the Pythagorean identity). This rewrites the integral into two pieces:
- One part involves tanxsec2x, which is a perfect candidate for u-substitution with u=tanx (since du=sec2xdx).
- The other part is just tanx, whose antiderivative is −log∣cosx∣.
This decomposition turns a messy trigonometric integral into clean, elementary forms.
Step-by-Step Solution
1. Rewrite the integrand using the identity.
Recall: tan2x=sec2x−1. So:
2tan3x=2tanx⋅tan2x=2tanx(sec2x−1)=2tanxsec2x−2tanx.
Thus the integral becomes:
∫0π/42tan3xdx=∫0π/42tanxsec2xdx−∫0π/42tanxdx.
2. Handle the first integral: I1=∫2tanxsec2xdx.
Let u=tanx. Then du=sec2xdx. The factor 2 is constant, so:
∫2tanxsec2xdx=2∫udu=2⋅2u2=u2=tan2x.
No constant needed since we'll evaluate definite limits. So:
I1=[tan2x]0π/4=tan2(4π)−tan2(0)=12−0=1.
The substitution u=tanx works because sec2x appears as the derivative — a classic pattern for integrals of the form ∫f(tanx)sec2xdx.
3. Handle the second integral: I2=∫2tanxdx.
We know ∫tanxdx=−log∣cosx∣+C. So:
∫2tanxdx=−2log∣cosx∣+C. …