1. Find the differential $\text{d}x$ and the new limits in terms of $\theta$.
Let x = tan θ x = \tan \theta x = tan θ .
Differentiating with respect to θ \theta θ :
d x d θ = sec 2 θ ⟹ d x = sec 2 θ d θ \frac{\text{d}x}{\text{d}\theta} = \sec^2 \theta \implies \text{d}x = \sec^2 \theta \text{ d}\theta d θ d x = sec 2 θ ⟹ d x = sec 2 θ d θ
Change of limits:
When x = 0 x = 0 x = 0 , tan θ = 0 ⟹ θ = 0 \tan \theta = 0 \implies \theta = 0 tan θ = 0 ⟹ θ = 0
When x = 1 x = 1 x = 1 , tan θ = 1 ⟹ θ = π 4 \tan \theta = 1 \implies \theta = \frac{\pi}{4} tan θ = 1 ⟹ θ = 4 π
2. Substitute $x$, $\text{d}x$, and the limits into the integral, and apply the Pythagorean identity.
Substituting into the integral:
∫ 0 1 x 3 ( x 2 + 1 ) 3 d x = ∫ 0 π 4 tan 3 θ ( tan 2 θ + 1 ) 3 sec 2 θ d θ \int_{0}^{1} \frac{x^3}{\left(x^2+1\right)^3} \text{ d}x = \int_{0}^{\frac{\pi}{4}} \frac{\tan^3 \theta}{\left(\tan^2 \theta + 1\right)^3} \sec^2 \theta \text{ d}\theta ∫ 0 1 ( x 2 + 1 ) 3 x 3 d x = ∫ 0 4 π ( t a n 2 θ + 1 ) 3 t a n 3 θ sec 2 θ d θ
Using the identity tan 2 θ + 1 = sec 2 θ \tan^2 \theta + 1 = \sec^2 \theta tan 2 θ + 1 = sec 2 θ :
= ∫ 0 π 4 tan 3 θ ( sec 2 θ ) 3 sec 2 θ d θ = \int_{0}^{\frac{\pi}{4}} \frac{\tan^3 \theta}{\left(\sec^2 \theta\right)^3} \sec^2 \theta \text{ d}\theta = ∫ 0 4 π ( s e c 2 θ ) 3 t a n 3 θ sec 2 θ d θ
= ∫ 0 π 4 tan 3 θ sec 6 θ sec 2 θ d θ = \int_{0}^{\frac{\pi}{4}} \frac{\tan^3 \theta}{\sec^6 \theta} \sec^2 \theta \text{ d}\theta = ∫ 0 4 π s e c 6 θ t a n 3 θ sec 2 θ d θ
= ∫ 0 π 4 tan 3 θ sec 4 θ d θ = \int_{0}^{\frac{\pi}{4}} \frac{\tan^3 \theta}{\sec^4 \theta} \text{ d}\theta = ∫ 0 4 π s e c 4 θ t a n 3 θ d θ
3. Simplify the trigonometric expression to show the target integrand.
Since tan θ = sin θ cos θ \tan \theta = \frac{\sin \theta}{\cos \theta} tan θ = c o s θ s i n θ and sec θ = 1 cos θ \sec \theta = \frac{1}{\cos \theta} sec θ = c o s θ 1 :
= ∫ 0 π 4 sin 3 θ cos 3 θ 1 cos 4 θ d θ = \int_{0}^{\frac{\pi}{4}} \frac{\frac{\sin^3 \theta}{\cos^3 \theta}}{\frac{1}{\cos^4 \theta}} \text{ d}\theta = ∫ 0 4 π c o s 4 θ 1 c o s 3 θ s i n 3 θ d θ
= ∫ 0 π 4 sin 3 θ cos 3 θ × cos 4 θ d θ = \int_{0}^{\frac{\pi}{4}} \frac{\sin^3 \theta}{\cos^3 \theta} \times \cos^4 \theta \text{ d}\theta = ∫ 0 4 π c o s 3 θ s i n 3 θ × cos 4 θ d θ
= ∫ 0 π 4 cos θ sin 3 θ d θ (shown) = \int_{0}^{\frac{\pi}{4}} \cos \theta \sin^3 \theta \text{ d}\theta \quad \text{(shown)} = ∫ 0 4 π cos θ sin 3 θ d θ (shown)
4. Integrate the simplified expression using the reverse chain rule.
To evaluate the integral, we can recognise it is of the form ∫ [ f ( θ ) ] n f ′ ( θ ) d θ \int [\mathrm{f}(\theta)]^n \mathrm{f}'(\theta) \text{ d}\theta ∫ [ f ( θ ) ] n f ′ ( θ ) d θ , since d d θ ( sin θ ) = cos θ \frac{\text{d}}{\text{d}\theta}(\sin \theta) = \cos \theta d θ d ( sin θ ) = cos θ :
∫ 0 π 4 sin 3 θ cos θ d θ = [ sin 4 θ 4 ] 0 π 4 \int_{0}^{\frac{\pi}{4}} \sin^3 \theta \cos \theta \text{ d}\theta = \left[ \frac{\sin^4 \theta}{4} \right]_0^{\frac{\pi}{4}} ∫ 0 4 π sin 3 θ cos θ d θ = [ 4 s i n 4 θ ] 0 4 π
5. Evaluate the integral at the upper and lower limits to find the exact value.
Substituting the limits:
= 1 4 ( sin π 4 ) 4 − 1 4 ( sin 0 ) 4 = \frac{1}{4} \left( \sin \frac{\pi}{4} \right)^4 - \frac{1}{4} \left( \sin 0 \right)^4 = 4 1 ( sin 4 π ) 4 − 4 1 ( sin 0 ) 4
= 1 4 ( 1 2 ) 4 − 0 = \frac{1}{4} \left( \frac{1}{\sqrt{2}} \right)^4 - 0 = 4 1 ( 2 1 ) 4 − 0
= 1 4 ( 1 4 ) = 1 16 = \frac{1}{4} \left( \frac{1}{4} \right) = \frac{1}{16} = 4 1 ( 4 1 ) = 16 1