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Exercise 7.7 · Q4

Q.Integrate the following function: x2+4x+1\sqrt{x^2+4x+1}

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The key idea is to rewrite the integrand by completing the square, then use a trigonometric substitution (secant) to handle the resulting u2−a2\sqrt{u^2 - a^2} form. The final result is 12(x+2)x2+4x+1−32log⁡∣x+2+x2+4x+1∣+C\frac{1}{2}(x+2)\sqrt{x^2+4x+1} - \frac{3}{2}\log\left|x+2+\sqrt{x^2+4x+1}\right| + C.

Why This Approach Works

When you see a quadratic inside a square root, your first instinct should be to complete the square. That turns the expression into something like (x+h)2±k\sqrt{(x+h)^2 \pm k}, which then suggests a trigonometric or hyperbolic substitution. Here, after completing the square, we get (x+2)2−3\sqrt{(x+2)^2 - 3}. That’s a perfect match for the secant substitution: u2−a2\sqrt{u^2 - a^2} with u=x+2u = x+2 and a=3a = \sqrt{3}. The secant substitution works because sec⁡2θ−1=tan⁡2θ\sec^2\theta - 1 = \tan^2\theta, which lets the square root simplify cleanly.

Let’s walk through it.

  1. Complete the square inside the radical. x2+4x+1=(x2+4x+4)−3=(x+2)2−3x^2+4x+1 = (x^2+4x+4) - 3 = (x+2)^2 - 3. So the integral becomes

∫(x+2)2−3 dx.\int \sqrt{(x+2)^2 - 3} \, dx.

  1. Set up the substitution. Let u=x+2u = x+2, so du=dxdu = dx. Then

∫u2−3 du.\int \sqrt{u^2 - 3} \, du.

This is of the form u2−a2\sqrt{u^2 - a^2} with a=3a = \sqrt{3}.

  1. Use the secant substitution. For u2−a2\sqrt{u^2 - a^2}, the standard trick is u=asec⁡θu = a \sec\theta, which gives du=asec⁡θtan⁡θ dθdu = a \sec\theta \tan\theta \, d\theta. Here a=3a = \sqrt{3}, so let u=3sec⁡θu = \sqrt{3} \sec\theta. Then du=3sec⁡θtan⁡θ dθdu = \sqrt{3} \sec\theta \tan\theta \, d\theta. Now

u2−3=3sec⁡2θ−3=3(sec⁡2θ−1)=3tan⁡2θ=3 ∣tan⁡θ∣.\sqrt{u^2 - 3} = \sqrt{3\sec^2\theta - 3} = \sqrt{3(\sec^2\theta - 1)} = \sqrt{3\tan^2\theta} = \sqrt{3}\,|\tan\theta|.

For the domain where the original integrand is defined (we’ll assume u≥3u \ge \sqrt{3} so θ∈[0,π/2)\theta \in [0, \pi/2)), tan⁡θ≥0\tan\theta \ge 0, so we can drop the absolute value:

u2−3=3tan⁡θ.\sqrt{u^2 - 3} = \sqrt{3} \tan\theta.

  1. Rewrite the integral in terms of θ\theta.

∫u2−3 du=∫(3tan⁡θ)⋅(3sec⁡θtan⁡θ dθ)=3∫sec⁡θtan⁡2θ dθ.\int \sqrt{u^2 - 3} \, du = \int (\sqrt{3} \tan\theta) \cdot (\sqrt{3} \sec\theta \tan\theta \, d\theta) = 3 \int \sec\theta \tan^2\theta \, d\theta.

  1. Simplify the trigonometric integral. Use tan⁡2θ=sec⁡2θ−1\tan^2\theta = \sec^2\theta - 1:

3∫sec⁡θ(sec⁡2θ−1) dθ=3∫(sec⁡3θ−sec⁡θ) dθ.3 \int \sec\theta (\sec^2\theta - 1) \, d\theta = 3 \int (\sec^3\theta - \sec\theta) \, d\theta.

Now we need two standard integrals:

  • ∫sec⁡θ dθ=log⁡∣sec⁡θ+tan⁡θ∣+C\int \sec\theta \, d\theta = \log|\sec\theta + \tan\theta| + C.
  • ∫sec⁡3θ dθ\int \sec^3\theta \, d\theta is a classic. Its derivation uses integration by parts:
    ›Proof

    Let I=∫sec⁡3θ dθI = \int \sec^3\theta \, d\theta. Write sec⁡3θ=sec⁡θ⋅sec⁡2θ\sec^3\theta = \sec\theta \cdot \sec^2\theta. Integrate by parts: let dv=sec⁡2θ dθdv = \sec^2\theta \, d\theta, u=sec⁡θu = \sec\theta. Then v=tan⁡θv = \tan\theta, du=sec⁡θtan⁡θ dθdu = \sec\theta \tan\theta \, d\theta.

    I=sec⁡θtan⁡θ−∫tan⁡θ⋅sec⁡θtan⁡θ dθ=sec⁡θtan⁡θ−∫sec⁡θtan⁡2θ dθ.I = \sec\theta \tan\theta - \int \tan\theta \cdot \sec\theta \tan\theta \, d\theta = \sec\theta \tan\theta - \int \sec\theta \tan^2\theta \, d\theta.

    Replace tan⁡2θ=sec⁡2θ−1\tan^2\theta = \sec^2\theta - 1:

    I=sec⁡θtan⁡θ−∫sec⁡θ(sec⁡2θ−1) dθ=sec⁡θtan⁡θ−∫sec⁡3θ dθ+∫sec⁡θ dθ.I = \sec\theta \tan\theta - \int \sec\theta (\sec^2\theta - 1) \, d\theta = \sec\theta \tan\theta - \int \sec^3\theta \, d\theta + \int \sec\theta \, d\theta.

    So I=sec⁡θtan⁡θ−I+log⁡∣sec⁡θ+tan⁡θ∣I = \sec\theta \tan\theta - I + \log|\sec\theta + \tan\theta|, giving 2I=sec⁡θtan⁡θ+log⁡∣sec⁡θ+tan⁡θ∣2I = \sec\theta \tan\theta + \log|\sec\theta + \tan\theta|, hence

    ∫sec⁡3θ dθ=12sec⁡θtan⁡θ+12log⁡∣sec⁡θ+tan⁡θ∣+C.\int \sec^3\theta \, d\theta = \frac{1}{2} \sec\theta \tan\theta + \frac{1}{2} \log|\sec\theta + \tan\theta| + C.

Using this,

3∫(sec⁡3θ−sec⁡θ) dθ=3(12sec⁡θtan⁡θ+12log⁡∣sec⁡θ+tan⁡θ∣−log⁡∣sec⁡θ+tan⁡θ∣)+C.3 \int (\sec^3\theta - \sec\theta) \, d\theta = 3\left( \frac{1}{2} \sec\theta \tan\theta + \frac{1}{2} \log|\sec\theta + \tan\theta| - \log|\sec\theta + \tan\theta| \right) + C.

Simplify:

=32sec⁡θtan⁡θ−32log⁡∣sec⁡θ+tan⁡θ∣+C.= \frac{3}{2} \sec\theta \tan\theta - \frac{3}{2} \log|\sec\theta + \tan\theta| + C.

  1. Back-substitute to uu (and then xx). Recall u=3sec⁡θu = \sqrt{3} \sec\theta, so sec⁡θ=u3\sec\theta = \frac{u}{\sqrt{3}}. Also tan⁡θ=sec⁡2θ−1=u23−1=u2−33\tan\theta = \sqrt{\sec^2\theta - 1} = \sqrt{\frac{u^2}{3} - 1} = \frac{\sqrt{u^2 - 3}}{\sqrt{3}}. …

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