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Exercise 7.7 · Q8

Q.Integrate the following function: x2+3x\sqrt{x^2+3x}

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The integral ∫x2+3x dx\int \sqrt{x^2+3x} \, dx is solved by completing the square inside the radical, then using a trigonometric substitution (secant) to simplify the expression. The final result is 12(x+32)x2+3x−98log⁡∣x+32+x2+3x∣+C\frac{1}{2}(x+\frac{3}{2})\sqrt{x^2+3x} - \frac{9}{8}\log\left|x+\frac{3}{2}+\sqrt{x^2+3x}\right| + C.

The key to integrating expressions like x2+3x\sqrt{x^2+3x} is to recognize that the quadratic under the square root can be rewritten as a perfect square plus a constant. This is the technique of completing the square. Once we have something like (x+a)2+b\sqrt{(x+a)^2 + b} or (x+a)2−b\sqrt{(x+a)^2 - b}, we can use a trigonometric substitution to eliminate the square root.

Why does this work? The identity sec⁡2θ−1=tan⁡2θ\sec^2\theta - 1 = \tan^2\theta is perfect for handling expressions of the form u2−a2\sqrt{u^2 - a^2}, because substituting u=asec⁡θu = a\sec\theta turns the square root into atan⁡θa\tan\theta, which is a simple trigonometric function. Similarly, sin⁡2\sin^2 and cos⁡2\cos^2 handle sums. Here, after completing the square, we get a difference of squares, so secant substitution is the right tool.

Let’s work through it step by step.

  1. Complete the square. The expression inside the square root is x2+3xx^2 + 3x. To complete the square, take half of the coefficient of xx (which is 32\frac{3}{2}), square it (94\frac{9}{4}), and add and subtract it:

x2+3x=(x2+3x+94)−94=(x+32)2−94.x^2 + 3x = \left(x^2 + 3x + \frac{9}{4}\right) - \frac{9}{4} = \left(x + \frac{3}{2}\right)^2 - \frac{9}{4}.

So the integral becomes:

∫(x+32)2−(32)2 dx.\int \sqrt{\left(x + \frac{3}{2}\right)^2 - \left(\frac{3}{2}\right)^2} \, dx.

  1. Make a substitution to simplify. Let u=x+32u = x + \frac{3}{2}, so du=dxdu = dx. Then the integral is:

∫u2−(32)2 du.\int \sqrt{u^2 - \left(\frac{3}{2}\right)^2} \, du.

This is now in the standard form ∫u2−a2 du\int \sqrt{u^2 - a^2} \, du with a=32a = \frac{3}{2}.

  1. Apply trigonometric substitution. For u2−a2\sqrt{u^2 - a^2}, we use u=asec⁡θu = a\sec\theta, so du=asec⁡θtan⁡θ dθdu = a\sec\theta\tan\theta \, d\theta. Here a=32a = \frac{3}{2}, so:

u=32sec⁡θ,du=32sec⁡θtan⁡θ dθ.u = \frac{3}{2}\sec\theta, \quad du = \frac{3}{2}\sec\theta\tan\theta \, d\theta.

Then u2−a2=94sec⁡2θ−94=32sec⁡2θ−1=32tan⁡θ\sqrt{u^2 - a^2} = \sqrt{\frac{9}{4}\sec^2\theta - \frac{9}{4}} = \frac{3}{2}\sqrt{\sec^2\theta - 1} = \frac{3}{2}\tan\theta (assuming tan⁡θ≥0\tan\theta \geq 0 for the principal branch; we’ll handle absolute values later).

The integral becomes:

∫(32tan⁡θ)⋅(32sec⁡θtan⁡θ)dθ=94∫sec⁡θtan⁡2θ dθ.\int \left(\frac{3}{2}\tan\theta\right) \cdot \left(\frac{3}{2}\sec\theta\tan\theta\right) d\theta = \frac{9}{4} \int \sec\theta \tan^2\theta \, d\theta.

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

94∫sec⁡θ(sec⁡2θ−1) dθ=94∫(sec⁡3θ−sec⁡θ) dθ.\frac{9}{4} \int \sec\theta (\sec^2\theta - 1) \, d\theta = \frac{9}{4} \int (\sec^3\theta - \sec\theta) \, d\theta.

Now we need to integrate sec⁡3θ\sec^3\theta and sec⁡θ\sec\theta. The integral of sec⁡θ\sec\theta is standard: ∫sec⁡θ dθ=log⁡∣sec⁡θ+tan⁡θ∣+C\int \sec\theta \, d\theta = \log|\sec\theta + \tan\theta| + C.

For sec⁡3θ\sec^3\theta, we use integration by parts or a known reduction formula. Let’s do it quickly:

∫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.

(This can be derived by writing ∫sec⁡3θ dθ=∫sec⁡θ⋅sec⁡2θ dθ\int \sec^3\theta \, d\theta = \int \sec\theta \cdot \sec^2\theta \, d\theta and integrating by parts with u=sec⁡θu = \sec\theta, dv=sec⁡2θ dθdv = \sec^2\theta \, d\theta.)

So:

94∫(sec⁡3θ−sec⁡θ) dθ=94[12sec⁡θtan⁡θ+12log⁡∣sec⁡θ+tan⁡θ∣−log⁡∣sec⁡θ+tan⁡θ∣]+C.\frac{9}{4} \int (\sec^3\theta - \sec\theta) \, d\theta = \frac{9}{4} \left[ \frac{1}{2}\sec\theta\tan\theta + \frac{1}{2}\log|\sec\theta + \tan\theta| - \log|\sec\theta + \tan\theta| \right] + C.

Simplify the log terms: 12log⁡∣⋯∣−log⁡∣⋯∣=−12log⁡∣sec⁡θ+tan⁡θ∣\frac{1}{2}\log|\cdots| - \log|\cdots| = -\frac{1}{2}\log|\sec\theta + \tan\theta|.

Thus:

94(12sec⁡θtan⁡θ−12log⁡∣sec⁡θ+tan⁡θ∣)+C=98sec⁡θtan⁡θ−98log⁡∣sec⁡θ+tan⁡θ∣+C.\frac{9}{4} \left( \frac{1}{2}\sec\theta\tan\theta - \frac{1}{2}\log|\sec\theta + \tan\theta| \right) + C = \frac{9}{8}\sec\theta\tan\theta - \frac{9}{8}\log|\sec\theta + \tan\theta| + C.

  1. Back-substitute to uu and then to xx. We have u=32sec⁡θu = \frac{3}{2}\sec\theta, so sec⁡θ=2u3\sec\theta = \frac{2u}{3}. Also, tan⁡θ=sec⁡2θ−1=4u29−1=23u2−94=23u2−a2\tan\theta = \sqrt{\sec^2\theta - 1} = \sqrt{\frac{4u^2}{9} - 1} = \frac{2}{3}\sqrt{u^2 - \frac{9}{4}} = \frac{2}{3}\sqrt{u^2 - a^2}. But note: u2−a2\sqrt{u^2 - a^2} is exactly the original square root we had! So tan⁡θ=23u2−94\tan\theta = \frac{2}{3}\sqrt{u^2 - \frac{9}{4}}. …

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