Difference between revisions of "The Substitution and Composition Theorems"

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     &= -\ln |\cos x| + C = \ln |\sec x| + C.
 
     &= -\ln |\cos x| + C = \ln |\sec x| + C.
 
  \end{align}</math>
 
  \end{align}</math>
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==Composition Theorem==
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Let <span class="math-inline"><math> f </math></span> be Riemann integrable on <span class="math-inline"><math> [a,b] </math></span>, with <span class="math-inline"><math> f([a,b]) \subseteq [c,d] </math></span>, and let <span class="math-inline"><math> \phi : [c,d]\to\R </math></span> be continuous. Then the composition <span class="math-inline"><math> \phi \circ f </math></span> is Riemann integrable on <span class="math-inline"><math> [a,b] </math></span> as well.
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==Product Theorem==
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==Licensing==
 
==Licensing==
 
Content obtained and/or adapted from:
 
Content obtained and/or adapted from:
 
* [https://en.wikipedia.org/wiki/Integration_by_substitution Integration by substitution, Wikipedia] under a CC BY-SA license
 
* [https://en.wikipedia.org/wiki/Integration_by_substitution Integration by substitution, Wikipedia] under a CC BY-SA license

Revision as of 16:30, 9 November 2021

Substitution Theorem

Definite integrals

Let φ : [a, b] → I be a differentiable function with a continuous derivative, where IR is an interval. Suppose that f : IR is a continuous function. Then

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_a^b f(\varphi(x))\varphi'(x)\, dx = \int_{\varphi(a)}^{\varphi(b)} f(u)\,du. }

In Leibniz notation, the substitution u = φ(x) yields

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{du}{dx} = \varphi'(x).}

Working heuristically with infinitesimals yields the equation

which suggests the substitution formula above. (This equation may be put on a rigorous foundation by interpreting it as a statement about differential forms.) One may view the method of integration by substitution as a partial justification of Leibniz's notation for integrals and derivatives.

The formula is used to transform one integral into another integral that is easier to compute. Thus, the formula can be read from left to right or from right to left in order to simplify a given integral. When used in the former manner, it is sometimes known as u-substitution or w-substitution in which a new variable is defined to be a function of the original variable found inside the composite function multiplied by the derivative of the inner function. The latter manner is commonly used in trigonometric substitution, replacing the original variable with a trigonometric function of a new variable and the original differential with the differential of the trigonometric function.

Proof

Integration by substitution can be derived from the fundamental theorem of calculus as follows. Let f and φ be two functions satisfying the above hypothesis that f is continuous on I and φ is integrable on the closed interval [a,b]. Then the function f(φ(x))φ′(x) is also integrable on [a,b]. Hence the integrals

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_a^b f(\varphi(x))\varphi'(x)\,dx}

and

in fact exist, and it remains to show that they are equal.

Since f is continuous, it has an antiderivative F. The composite function Fφ is then defined. Since φ is differentiable, combining the chain rule and the definition of an antiderivative gives

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle (F \circ \varphi)'(x) = F'(\varphi(x))\varphi'(x) = f(\varphi(x))\varphi'(x).}

Applying the fundamental theorem of calculus twice gives

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} \int_a^b f(\varphi(x))\varphi'(x)\,dx &= \int_a^b (F \circ \varphi)'(x)\,dx \\ &= (F \circ \varphi)(b) - (F \circ \varphi)(a) \\ &= F(\varphi(b)) - F(\varphi(a)) \\ &= \int_{\varphi(a)}^{\varphi(b)} f(u)\,du, \end{align} }

which is the substitution rule.

Examples

Example 1

Consider the integral

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_0^2 x \cos(x^2+1) dx.}

Make the substitution Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u = x^{2} + 1} to obtain , meaning Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \textstyle xdx = \frac{1}{2}du} . Therefore,

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} \int_{x=0}^{x=2} x \cos(x^2+1) dx &= \frac{1}{2} \int_{u=1}^{u=5}\cos(u)\,du \\[6pt] &= \frac{1}{2}(\sin(5)-\sin(1)). \end{align}}

Since the lower limit Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x = 0} was replaced with Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u = 1} , and the upper limit with Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 2^{2} + 1 = 5} , a transformation back into terms of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x} was unnecessary.

Alternatively, one may fully evaluate the indefinite integral first then apply the boundary conditions. This becomes especially handy when multiple substitutions are used.

Example 2

For the integral

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_0^1 \sqrt{1-x^2}\,dx,}

a variation of the above procedure is needed. The substitution Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x = \sin u } implying is useful because Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sqrt{1-\sin^2u} = \cos(u)} . We thus have

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} \int_0^1 \sqrt{1-x^2}\,dx &= \int_0^{\pi/2} \sqrt{1-\sin^2u} \cos(u)\,du \\[6pt] &= \int_0^{\pi/2} \cos^2u\,du \\[6pt] &= \left[\frac{u}{2} + \frac{\sin(2u)}{4}\right]\Biggl|_0^{\pi/2} \\[6pt] &= \frac{\pi}{4} + 0 = \frac{\pi}{4}. \end{align}}

The resulting integral can be computed using integration by parts or a double angle formula, , followed by one more substitution. One can also note that the function being integrated is the upper right quarter of a circle with a radius of one, and hence integrating the upper right quarter from zero to one is the geometric equivalent to the area of one quarter of the unit circle, or Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \pi / 4 } .

Indefinite Integrals

Substitution can be used to determine antiderivatives. One chooses a relation between Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x} and , determines the corresponding relation between Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle dx} and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle du} by differentiating, and performs the substitutions. An antiderivative for the substituted function can hopefully be determined; the original substitution between and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u} is then undone.

Similar to example 1 above, the following antiderivative can be obtained with this method:

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} \int x \cos(x^2+1) \,dx &= \frac{1}{2} \int 2x \cos(x^2+1) \,dx \\[6pt] &= \frac{1}{2} \int\cos u\,du \\[6pt] &= \frac{1}{2}\sin u + C = \frac{1}{2}\sin(x^2+1) + C, \end{align}}

where Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle C} is an arbitrary constant of integration.

There were no integral boundaries to transform, but in the last step reverting the original substitution Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u = x^{2} + 1} was necessary. When evaluating definite integrals by substitution, one may calculate the antiderivative fully first, then apply the boundary conditions. In that case, there is no need to transform the boundary terms.

The tangent function can be integrated using substitution by expressing it in terms of the sine and cosine:

Using the substitution Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u = \cos x} gives Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle du = -\sin x\,dx} and

Composition Theorem

Let Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle f } be Riemann integrable on Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle [a,b] } , with , and let Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi : [c,d]\to\R } be continuous. Then the composition Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi \circ f } is Riemann integrable on as well.

Product Theorem

Licensing

Content obtained and/or adapted from: