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Exercise 7.6 · Q21

Q.Integrate the following function: e2xsin⁡xe^{2x} \sin x

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The integral of e2xsin⁡xe^{2x} \sin x is found using integration by parts twice, which creates a cyclic equation that we solve algebraically. The final result is e2x5(2sin⁡x−cos⁡x)+C\frac{e^{2x}}{5}(2\sin x - \cos x) + C.

Why This Approach Works

When you see a product of an exponential and a trigonometric function, your first instinct might be to try substitution — but that won't help here because neither function is the derivative of the other in a simple way. The key insight is that integration by parts can reduce the complexity step by step, but because both e2xe^{2x} and sin⁡x\sin x are "cyclic" under differentiation (they loop back to themselves after two derivatives), we end up with the original integral reappearing. That lets us treat it as an algebraic equation and solve for the unknown integral.

Tip

This "recurring integral" trick works for any pair of functions that are each other's derivatives up to a constant factor — like eaxsin⁡(bx)e^{ax}\sin(bx) or eaxcos⁡(bx)e^{ax}\cos(bx). You never need to memorize a formula; just set up the equation.

Step-by-Step Solution

  1. Set up the integral and choose parts.

    Let I=∫e2xsin⁡x dxI = \int e^{2x} \sin x \, dx.

    For integration by parts, we need uu and dvdv. A good rule: pick uu as the function that simplifies when differentiated. Here, both e2xe^{2x} and sin⁡x\sin x are fine, but let's choose:

    u=sin⁡xu = \sin x, dv=e2xdxdv = e^{2x} dx.

    Then du=cos⁡x dxdu = \cos x \, dx, and v=∫e2xdx=12e2xv = \int e^{2x} dx = \frac{1}{2} e^{2x}.

  2. Apply integration by parts the first time.

    The formula ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du gives:

I=sin⁡x⋅12e2x−∫12e2xcos⁡x dx=12e2xsin⁡x−12∫e2xcos⁡x dx.I = \sin x \cdot \frac{1}{2} e^{2x} - \int \frac{1}{2} e^{2x} \cos x \, dx = \frac{1}{2} e^{2x} \sin x - \frac{1}{2} \int e^{2x} \cos x \, dx.

  1. Now we need ∫e2xcos⁡x dx\int e^{2x} \cos x \, dx — call it JJ. Apply integration by parts again to JJ. This time, let u=cos⁡xu = \cos x, dv=e2xdxdv = e^{2x} dx. Then du=−sin⁡x dxdu = -\sin x \, dx, v=12e2xv = \frac{1}{2} e^{2x}. So:

J=cos⁡x⋅12e2x−∫12e2x(−sin⁡x) dx=12e2xcos⁡x+12∫e2xsin⁡x dx.J = \cos x \cdot \frac{1}{2} e^{2x} - \int \frac{1}{2} e^{2x} (-\sin x) \, dx = \frac{1}{2} e^{2x} \cos x + \frac{1}{2} \int e^{2x} \sin x \, dx.

  1. Notice the original integral II has reappeared. The last term is exactly 12I\frac{1}{2} I. So we have:

J=12e2xcos⁡x+12I.J = \frac{1}{2} e^{2x} \cos x + \frac{1}{2} I.

  1. Substitute JJ back into the expression for II. From step 2: I=12e2xsin⁡x−12JI = \frac{1}{2} e^{2x} \sin x - \frac{1}{2} J. Replace JJ: I=12e2xsin⁡x−12(12e2xcos⁡x+12I).I = \frac{1}{2} e^{2x} \sin x - \frac{1}{2} \left( \frac{1}{2} e^{2x} \cos x + \frac{1}{2} I \right). …

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