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Calculus - Integration by substitution

Grade 11IB_AA

Review the key concepts, formulae, and examples before starting your quiz.

πŸ”‘Concepts

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Integration by substitution is a method used to find antiderivatives by reversing the Chain Rule. It is particularly useful when the integrand contains a function g(x)g(x) and its derivative gβ€²(x)g'(x).

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The core idea is to introduce a new variable u=g(x)u = g(x), which simplifies the integral into a standard form ∫f(u)du\int f(u) du.

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When performing substitution, the differential dxdx must also be converted to dudu using the relationship du=gβ€²(x)dxdu = g'(x) dx or dx=dugβ€²(x)dx = \frac{du}{g'(x)}.

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For definite integrals ∫abf(g(x))gβ€²(x)dx\int_{a}^{b} f(g(x))g'(x) dx, the limits of integration must be updated from xx-values to uu-values using the substitution u=g(x)u = g(x). If limits are updated, back-substitution is not required.

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Common substitution patterns include ∫[f(x)]nfβ€²(x)dx\int [f(x)]^n f'(x) dx, ∫fβ€²(x)f(x)dx\int \frac{f'(x)}{f(x)} dx, and ∫ef(x)fβ€²(x)dx\int e^{f(x)} f'(x) dx.

πŸ“Formulae

∫f(g(x))gβ€²(x)dx=∫f(u)duΒ whereΒ u=g(x)\int f(g(x)) g'(x) dx = \int f(u) du \text{ where } u = g(x)

∫abf(g(x))gβ€²(x)dx=∫g(a)g(b)f(u)du\int_{a}^{b} f(g(x)) g'(x) dx = \int_{g(a)}^{g(b)} f(u) du

∫[g(x)]ngβ€²(x)dx=[g(x)]n+1n+1+C,nβ‰ βˆ’1\int [g(x)]^n g'(x) dx = \frac{[g(x)]^{n+1}}{n+1} + C, \quad n \neq -1

∫gβ€²(x)g(x)dx=ln⁑∣g(x)∣+C\int \frac{g'(x)}{g(x)} dx = \ln|g(x)| + C

∫eg(x)gβ€²(x)dx=eg(x)+C\int e^{g(x)} g'(x) dx = e^{g(x)} + C

πŸ’‘Examples

Problem 1:

Evaluate the indefinite integral ∫3x2(x3+5)4dx\int 3x^2(x^3 + 5)^4 dx.

Solution:

Let u=x3+5u = x^3 + 5. Then dudx=3x2\frac{du}{dx} = 3x^2, which implies du=3x2dxdu = 3x^2 dx. Substitute uu and dudu into the integral: ∫u4du\int u^4 du Integrate with respect to uu: u55+C\frac{u^5}{5} + C Substitute back u=x3+5u = x^3 + 5: (x3+5)55+C\frac{(x^3 + 5)^5}{5} + C

Explanation:

We identify x3+5x^3+5 as the inner function because its derivative 3x23x^2 is present as a factor in the integrand.

Problem 2:

Find the exact value of ∫01xex2dx\int_{0}^{1} x e^{x^2} dx.

Solution:

Let u=x2u = x^2. Then du=2xdxdu = 2x dx, so xdx=12dux dx = \frac{1}{2} du. Change the limits of integration: When x=0x = 0, u=02=0u = 0^2 = 0. When x=1x = 1, u=12=1u = 1^2 = 1. Substitute into the integral: ∫01euβ‹…12du=12∫01eudu\int_{0}^{1} e^u \cdot \frac{1}{2} du = \frac{1}{2} \int_{0}^{1} e^u du Evaluate the integral: 12[eu]01=12(e1βˆ’e0)\frac{1}{2} [e^u]_{0}^{1} = \frac{1}{2} (e^1 - e^0) Final Answer: 12(eβˆ’1)Β orΒ eβˆ’12\frac{1}{2}(e - 1) \text{ or } \frac{e-1}{2}

Explanation:

Since the derivative of x2x^2 is 2x2x, and we have an xx term, we use u=x2u=x^2. Note the change of limits to keep the integral entirely in terms of uu.

Problem 3:

Evaluate ∫tan⁑(x)dx\int \tan(x) dx.

Solution:

Rewrite tan⁑(x)\tan(x) as sin⁑(x)cos⁑(x)\frac{\sin(x)}{\cos(x)}: ∫sin⁑(x)cos⁑(x)dx\int \frac{\sin(x)}{\cos(x)} dx Let u=cos⁑(x)u = \cos(x). Then du=βˆ’sin⁑(x)dxdu = -\sin(x) dx, so sin⁑(x)dx=βˆ’du\sin(x) dx = -du. Substitute: βˆ«βˆ’1udu=βˆ’ln⁑∣u∣+C\int \frac{-1}{u} du = -\ln|u| + C Substitute back u=cos⁑(x)u = \cos(x): βˆ’ln⁑∣cos⁑(x)∣+C-\ln|\cos(x)| + C Using log properties, this can also be written as: ln⁑∣sec⁑(x)∣+C\ln|\sec(x)| + C

Explanation:

This example uses the fβ€²(x)f(x)\frac{f'(x)}{f(x)} pattern where the numerator is the derivative of the denominator (with a sign change).