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Identify the form of the integral.

Mathematics

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Step-by-step solution

6 steps

To solve the integral ∫x2−a2 dx\int \sqrt{x^2 - a^2} \, dx:

  1. Identify the form of the integral.

    This integral is of the form ∫x2−a2 dx\int \sqrt{x^2 - a^2} \, dx, which suggests using a trigonometric substitution.

  2. Choose the appropriate trigonometric substitution.

    For expressions involving x2−a2\sqrt{x^2 - a^2}, the standard substitution is x=asec⁡θx = a \sec \theta.
    From this substitution, we can find dxdx:

    dx=asec⁡θtan⁡θ dθdx = a \sec \theta \tan \theta \, d\theta

    Also, we can express x2−a2\sqrt{x^2 - a^2} in terms of θ\theta:

    x2−a2=(asec⁡θ)2−a2=a2sec⁡2θ−a2\sqrt{x^2 - a^2} = \sqrt{(a \sec \theta)^2 - a^2} = \sqrt{a^2 \sec^2 \theta - a^2} =a2(sec⁡2θ−1)=a2tan⁡2θ=a∣tan⁡θ∣= \sqrt{a^2 (\sec^2 \theta - 1)} = \sqrt{a^2 \tan^2 \theta} = a |\tan \theta|

    Assuming x>ax > a (or x<−ax < -a) and θ\theta is in an appropriate range where tan⁡θ≥0\tan \theta \ge 0, we have x2−a2=atan⁡θ\sqrt{x^2 - a^2} = a \tan \theta.

  3. Substitute into the integral.

    ∫(atan⁡θ)(asec⁡θtan⁡θ) dθ\int (a \tan \theta) (a \sec \theta \tan \theta) \, d\theta ∫a2tan⁡2θsec⁡θ dθ\int a^2 \tan^2 \theta \sec \theta \, d\theta
  4. Rewrite tan⁡2θ\tan^2 \theta using the identity tan⁡2θ=sec⁡2θ−1\tan^2 \theta = \sec^2 \theta - 1.

    ∫a2(sec⁡2θ−1)sec⁡θ dθ\int a^2 (\sec^2 \theta - 1) \sec \theta \, d\theta a2∫(sec⁡3θ−sec⁡θ) dθa^2 \int (\sec^3 \theta - \sec \theta) \, d\theta a2(∫sec⁡3θ dθ−∫sec⁡θ dθ)a^2 \left( \int \sec^3 \theta \, d\theta - \int \sec \theta \, d\theta \right)
  5. Evaluate the standard integrals.

    We use the known integral formulas:

    ∫sec⁡θ dθ=ln⁡∣sec⁡θ+tan⁡θ∣+C1\int \sec \theta \, d\theta = \ln|\sec \theta + \tan \theta| + C_1 ∫sec⁡3θ dθ=12sec⁡θtan⁡θ+12ln⁡∣sec⁡θ+tan⁡θ∣+C2\int \sec^3 \theta \, d\theta = \frac{1}{2} \sec \theta \tan \theta + \frac{1}{2} \ln|\sec \theta + \tan \theta| + C_2

    Substitute these back into the expression:

    a2((12sec⁡θtan⁡θ+12ln⁡∣sec⁡θ+tan⁡θ∣)−ln⁡∣sec⁡θ+tan⁡θ∣)+Ca^2 \left( \left( \frac{1}{2} \sec \theta \tan \theta + \frac{1}{2} \ln|\sec \theta + \tan \theta| \right) - \ln|\sec \theta + \tan \theta| \right) + C a2(12sec⁡θtan⁡θ−12ln⁡∣sec⁡θ+tan⁡θ∣)+Ca^2 \left( \frac{1}{2} \sec \theta \tan \theta - \frac{1}{2} \ln|\sec \theta + \tan \theta| \right) + C a22(sec⁡θtan⁡θ−ln⁡∣sec⁡θ+tan⁡θ∣)+C\frac{a^2}{2} (\sec \theta \tan \theta - \ln|\sec \theta + \tan \theta|) + C
  6. Convert back to xx.

    From x=asec⁡θx = a \sec \theta, we have sec⁡θ=xa\sec \theta = \frac{x}{a}.
    To find tan⁡θ\tan \theta, we use the identity tan⁡θ=sec⁡2θ−1\tan \theta = \sqrt{\sec^2 \theta - 1}:

    tan⁡θ=(xa)2−1=x2a2−1=x2−a2a2=x2−a2a\tan \theta = \sqrt{\left(\frac{x}{a}\right)^2 - 1} = \sqrt{\frac{x^2}{a^2} - 1} = \sqrt{\frac{x^2 - a^2}{a^2}} = \frac{\sqrt{x^2 - a^2}}{a}

    Now substitute these expressions back into the result:

    a22(xa⋅x2−a2a−ln⁡∣xa+x2−a2a∣)+C\frac{a^2}{2} \left( \frac{x}{a} \cdot \frac{\sqrt{x^2 - a^2}}{a} - \ln\left|\frac{x}{a} + \frac{\sqrt{x^2 - a^2}}{a}\right| \right) + C a22(xx2−a2a2−ln⁡∣x+x2−a2a∣)+C\frac{a^2}{2} \left( \frac{x \sqrt{x^2 - a^2}}{a^2} - \ln\left|\frac{x + \sqrt{x^2 - a^2}}{a}\right| \right) + C

    Distribute a22\frac{a^2}{2}:

    xx2−a22−a22ln⁡∣x+x2−a2a∣+C\frac{x \sqrt{x^2 - a^2}}{2} - \frac{a^2}{2} \ln\left|\frac{x + \sqrt{x^2 - a^2}}{a}\right| + C

    Using the logarithm property ln⁡∣AB∣=ln⁡∣A∣−ln⁡∣B∣\ln\left|\frac{A}{B}\right| = \ln|A| - \ln|B|:

    xx2−a22−a22(ln⁡∣x+x2−a2∣−ln⁡∣a∣)+C\frac{x \sqrt{x^2 - a^2}}{2} - \frac{a^2}{2} (\ln|x + \sqrt{x^2 - a^2}| - \ln|a|) + C xx2−a22−a22ln⁡∣x+x2−a2∣+a22ln⁡∣a∣+C\frac{x \sqrt{x^2 - a^2}}{2} - \frac{a^2}{2} \ln|x + \sqrt{x^2 - a^2}| + \frac{a^2}{2} \ln|a| + C

    Since a22ln⁡∣a∣\frac{a^2}{2} \ln|a| is a constant, it can be absorbed into the arbitrary constant CC.

    The final answer is x2x2−a2−a22ln⁡∣x+x2−a2∣+C\boxed{\frac{x}{2}\sqrt{x^2 - a^2} - \frac{a^2}{2}\ln|x + \sqrt{x^2 - a^2}| + C}.

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