Integration
Integration is the inverse operation of differentiation. Given the derivative of a function,
integration recovers the original function (up to an additive constant). It is a central operation
in calculus with wide-ranging applications in geometry, physics, and probability.
Two principal forms exist:
Indefinite integration (antidifferentiation): finds the general antiderivative of a function,
producing a family of functions differing by a constant.
Definite integration : computes a numerical value representing the signed area under a curve
between two limits.
These are linked by the Fundamental Theorem of Calculus, which unifies differentiation and
integration into a single coherent framework.
Notation
∫ f ( x ) d x = F ( x ) + C \int f(x)\,dx = F(x) + C ∫ f ( x ) d x = F ( x ) + C
where F ′ ( x ) = f ( x ) F'(x) = f(x) F ′ ( x ) = f ( x ) and C C C is the constant of integration. The symbol ∫ \int ∫ is an elongated S S S
(for "sum"), f ( x ) f(x) f ( x ) is the integrand, and d x dx d x indicates the variable of integration.
1. Antiderivatives
Definition
A function F F F is an antiderivative of f f f on an interval I I I if F ′ ( x ) = f ( x ) F'(x) = f(x) F ′ ( x ) = f ( x ) for all x ∈ I x \in I x ∈ I .
If F F F is an antiderivative of f f f , then so is F + C F + C F + C for any constant C ∈ ′ { ′ R ′ } ′ C \in \mathbb{'\{'}R{'\}'} C ∈ ′ { ′ R ′ } ′ .
Basic Rules
Power Rule
For n ≠ − 1 n \neq -1 n = − 1 :
∫ x n d x = x n + 1 n + 1 + C \int x^n\,dx = \frac{x^{n+1}}{n+1} + C ∫ x n d x = n + 1 x n + 1 + C
Constant Multiple Rule
For k ∈ ′ { ′ R ′ } ′ k \in \mathbb{'\{'}R{'\}'} k ∈ ′ { ′ R ′ } ′ :
∫ k f ( x ) d x = k ∫ f ( x ) d x \int k f(x)\,dx = k \int f(x)\,dx ∫ k f ( x ) d x = k ∫ f ( x ) d x
Sum and Difference Rule
∫ [ f ( x ) ± g ( x ) ] d x = ∫ f ( x ) d x ± ∫ g ( x ) d x \int [f(x) \pm g(x)]\,dx = \int f(x)\,dx \pm \int g(x)\,dx ∫ [ f ( x ) ± g ( x )] d x = ∫ f ( x ) d x ± ∫ g ( x ) d x
Reciprocal Rule (Logarithmic)
∫ 1 x d x = ln ∣ x ∣ + C \int \frac{1}{x}\,dx = \ln|x| + C ∫ x 1 d x = ln ∣ x ∣ + C
Common Antiderivatives
| f ( x ) f(x) f ( x ) | ∫ f ( x ) d x \int f(x)\,dx ∫ f ( x ) d x |
| -------------------------- | -------------------------------------------- | ------ | ---- |
| k k k | k x + C kx + C k x + C | | |
| x n x^n x n | x n + 1 n + 1 + C ( n ≠ − 1 ) \dfrac{x^{n+1}}{n+1} + C \quad (n \neq -1) n + 1 x n + 1 + C ( n = − 1 ) | | |
| 1 x \dfrac{1}{x} x 1 | ln ∣ x ∣ + C \ln | x | + C ln ∣ x ∣ + C |
| e x e^x e x | e x + C e^x + C e x + C | | |
| a x a^x a x | a x ln a + C \dfrac{a^x}{\ln a} + C ln a a x + C | | |
| sin x \sin x sin x | − cos x + C -\cos x + C − cos x + C | | |
| cos x \cos x cos x | sin x + C \sin x + C sin x + C | | |
| sec 2 x \sec^2 x sec 2 x | tan x + C \tan x + C tan x + C | | |
| csc 2 x \csc^2 x csc 2 x | − cot x + C -\cot x + C − cot x + C | | |
| sec x tan x \sec x \tan x sec x tan x | sec x + C \sec x + C sec x + C | | |
| csc x cot x \csc x \cot x csc x cot x | − csc x + C -\csc x + C − csc x + C | | |
| tan x \tan x tan x | ln ∣ sec x ∣ + C \ln | \sec x | + C ln ∣ sec x ∣ + C |
| cot x \cot x cot x | ln ∣ sin x ∣ + C \ln | \sin x | + C ln ∣ sin x ∣ + C |
| 1 1 − x 2 \frac{1}{\sqrt{1 - x^2}} 1 − x 2 1 | arcsin x + C \arcsin x + C arcsin x + C | | |
| 1 1 + x 2 \frac{1}{1 + x^2} 1 + x 2 1 | arctan x + C \arctan x + C arctan x + C | | |
Details
Expand
Find ∫ ( 3 x 4 − 5 x 2 + 7 ) d x \int (3x^4 - 5x^2 + 7)\,dx ∫ ( 3 x 4 − 5 x 2 + 7 ) d x
\begin`\{aligned}`
\int (3x^4 - 5x^2 + 7)\,dx &= 3 \cdot \frac{x^5}{5} - 5 \cdot \frac{x^3}{3} + 7x + C \\[6pt]
&= \frac{3x^5}{5} - \frac{5x^3}{3} + 7x + C
\end`\{aligned}` Find ∫ ( 2 x + 3 e x − 1 cos 2 x ) d x \int \left(\frac{2}{x} + 3e^x - \frac{1}{\cos^2 x}\right)\,dx ∫ ( x 2 + 3 e x − c o s 2 x 1 ) d x
\begin`\{aligned}`
\int \left(\frac{2}{x} + 3e^x - \sec^2 x\right)\,dx &= 2\ln|x| + 3e^x - \tan x + C
\end`\{aligned}`
2. Definite Integration
Definite Integral as a Limit of a Riemann Sum
For a function f f f continuous on [ a , b ] [a, b] [ a , b ] , the definite integral is defined as:
∫ a b f ( x ) d x = lim n → ∞ ∑ i = 1 n f ( x i ∗ ) Δ x \int_a^b f(x)\,dx = \lim_{n \to \infty} \sum_{i=1}^{n} f(x_i^*) \Delta x ∫ a b f ( x ) d x = n → ∞ lim i = 1 ∑ n f ( x i ∗ ) Δ x
where Δ x = b − a n \Delta x = \dfrac{b - a}{n} Δ x = n b − a and x i ∗ x_i^* x i ∗ is a sample point in the i i i -th subinterval.
Fundamental Theorem of Calculus -- Part 1
If f f f is continuous on [ a , b ] [a, b] [ a , b ] and F F F is defined by:
F ( x ) = ∫ a x f ( t ) d t F(x) = \int_a^x f(t)\,dt F ( x ) = ∫ a x f ( t ) d t
then F F F is differentiable on ( a , b ) (a, b) ( a , b ) and:
F ′ ( x ) = f ( x ) F'(x) = f(x) F ′ ( x ) = f ( x )
This establishes that differentiation and integration are inverse operations.
Fundamental Theorem of Calculus -- Part 2 (Evaluation Theorem)
If f f f is continuous on [ a , b ] [a, b] [ a , b ] and F F F is any antiderivative of f f f , then:
∫ a b f ( x ) d x = F ( b ) − F ( a ) \int_a^b f(x)\,dx = F(b) - F(a) ∫ a b f ( x ) d x = F ( b ) − F ( a )
This is typically written using bracket notation:
∫ a b f ( x ) d x = [ F ( x ) ] a b = F ( b ) − F ( a ) \int_a^b f(x)\,dx = \Big[F(x)\Big]_a^b = F(b) - F(a) ∫ a b f ( x ) d x = [ F ( x ) ] a b = F ( b ) − F ( a )
Area Under a Curve
If f ( x ) ≥ 0 f(x) \geq 0 f ( x ) ≥ 0 on [ a , b ] [a, b] [ a , b ] , then ∫ a b f ( x ) d x \int_a^b f(x)\,dx ∫ a b f ( x ) d x gives the area between the curve y = f ( x ) y = f(x) y = f ( x ) ,
the x x x -axis, and the vertical lines x = a x = a x = a and x = b x = b x = b .
If f ( x ) f(x) f ( x ) changes sign on [ a , b ] [a, b] [ a , b ] , the integral gives the net (signed) area. The total area is
computed by splitting at the zeros of f f f and taking absolute values:
T o t a l a r e a = ∫ a b ∣ f ( x ) ∣ d x \mathrm{Total area} = \int_a^b |f(x)|\,dx Totalarea = ∫ a b ∣ f ( x ) ∣ d x
Integration as Area Under a Curve
Adjust the sliders to change the function and limits, and observe how the shaded area approximates
the definite integral.
Details
Expand
Evaluate ∫ 1 3 ( x 2 + 1 ) d x \int_1^3 (x^2 + 1)\,dx ∫ 1 3 ( x 2 + 1 ) d x
\begin`\{aligned}`
\int_1^3 (x^2 + 1)\,dx &= \left[\frac{x^3}{3} + x\right]_1^3 \\[6pt]
&= \left(\frac{27}{3} + 3\right) - \left(\frac{1}{3} + 1\right) \\[6pt]
&= 12 - \frac{4}{3} = \frac{32}{3}
\end`\{aligned}` Find the area enclosed by y = x 2 − 4 y = x^2 - 4 y = x 2 − 4 and the x x x -axis.
The curve crosses the x x x -axis at x = − 2 x = -2 x = − 2 and x = 2 x = 2 x = 2 .
\begin`\{aligned}`
\mathrm{Area} &= \int_{-2}^2 |x^2 - 4|\,dx = \int_{-2}^2 (4 - x^2)\,dx \\[6pt]
&= \left[4x - \frac{x^3}{3}\right]_{-2}^2 \\[6pt]
&= \left(8 - \frac{8}{3}\right) - \left(-8 + \frac{8}{3}\right) = \frac{32}{3}
\end`\{aligned}`
3. Integration Techniques
3.1 Substitution (u u u -Substitution)
Substitution is the reverse of the chain rule. Given an integral containing a composite function,
choose a substitution u = g ( x ) u = g(x) u = g ( x ) such that d u = g ′ ( x ) d x du = g'(x)\,dx d u = g ′ ( x ) d x transforms the integral into a simpler
form.
General procedure:
Identify an inner function and set u = g ( x ) u = g(x) u = g ( x ) .
Compute d u = g ′ ( x ) d x du = g'(x)\,dx d u = g ′ ( x ) d x and solve for d x dx d x .
Rewrite the entire integral in terms of u u u .
Evaluate the integral with respect to u u u .
Substitute back x x x (for indefinite integrals) or change the limits (for definite integrals).
Changing limits for definite integrals:
∫ a b f ( g ( x ) ) g ′ ( x ) d x = ∫ g ( a ) g ( b ) f ( u ) d u \int_a^b f(g(x))\,g'(x)\,dx = \int_{g(a)}^{g(b)} f(u)\,du ∫ a b f ( g ( x )) g ′ ( x ) d x = ∫ g ( a ) g ( b ) f ( u ) d u
Details
Expand
Find ∫ 2 x x 2 + 1 d x \int 2x\sqrt{x^2 + 1}\,dx ∫ 2 x x 2 + 1 d x
Let u = x 2 + 1 u = x^2 + 1 u = x 2 + 1 , then d u = 2 x d x du = 2x\,dx d u = 2 x d x .
∫ 2 x x 2 + 1 d x = ∫ u d u = 2 3 u 3 / 2 + C = 2 3 ( x 2 + 1 ) 3 / 2 + C \int 2x\sqrt{x^2 + 1}\,dx = \int \sqrt{u}\,du = \frac{2}{3}u^{3/2} + C = \frac{2}{3}(x^2 + 1)^{3/2} + C ∫ 2 x x 2 + 1 d x = ∫ u d u = 3 2 u 3/2 + C = 3 2 ( x 2 + 1 ) 3/2 + C Evaluate ∫ 0 2 x x 2 + 1 d x \int_0^2 \frac{x}{x^2 + 1}\,dx ∫ 0 2 x 2 + 1 x d x
Let u = x 2 + 1 u = x^2 + 1 u = x 2 + 1 , d u = 2 x d x du = 2x\,dx d u = 2 x d x . When x = 0 x = 0 x = 0 , u = 1 u = 1 u = 1 ; when x = 2 x = 2 x = 2 , u = 5 u = 5 u = 5 .
∫ 0 2 x x 2 + 1 d x = 1 2 ∫ 1 5 1 u d u = 1 2 [ ln ∣ u ∣ ] 1 5 = 1 2 ln 5 \int_0^2 \frac{x}{x^2 + 1}\,dx = \frac{1}{2}\int_1^5 \frac{1}{u}\,du = \frac{1}{2}\Big[\ln|u|\Big]_1^5 = \frac{1}{2}\ln 5 ∫ 0 2 x 2 + 1 x d x = 2 1 ∫ 1 5 u 1 d u = 2 1 [ ln ∣ u ∣ ] 1 5 = 2 1 ln 5
3.2 Integration by Parts
Integration by parts is the reverse of the product rule. The formula is:
∫ u d v = u v − ∫ v d u \int u\,dv = uv - \int v\,du ∫ u d v = uv − ∫ v d u
Choosing u u u and d v dv d v : Use the LIATE priority rule (Logarithmic, Inverse trigonometric,
Algebraic, Trigonometric, Exponential) to select u u u as the function that appears first in the list.
Integration by parts may need to be applied repeatedly. For integrals of the form
∫ e a x sin ( b x ) d x \int e^{ax}\sin(bx)\,dx ∫ e a x sin ( b x ) d x or ∫ e a x cos ( b x ) d x \int e^{ax}\cos(bx)\,dx ∫ e a x cos ( b x ) d x , apply integration by parts twice and solve
the resulting equation algebraically.
Tabular (DI) method: For integrals of the form ∫ f ( x ) g ( x ) d x \int f(x) g(x)\,dx ∫ f ( x ) g ( x ) d x where one factor
differentiates to zero after finitely many steps, the tabular method provides an efficient
alternative to repeated application of the formula.
Details
Expand
Find ∫ x e x d x \int x e^x\,dx ∫ x e x d x
Let u = x u = x u = x , d v = e x d x dv = e^x\,dx d v = e x d x . Then d u = d x du = dx d u = d x and v = e x v = e^x v = e x .
∫ x e x d x = x e x − ∫ e x d x = x e x − e x + C = ( x − 1 ) e x + C \int x e^x\,dx = xe^x - \int e^x\,dx = xe^x - e^x + C = (x - 1)e^x + C ∫ x e x d x = x e x − ∫ e x d x = x e x − e x + C = ( x − 1 ) e x + C Find ∫ x 2 sin x d x \int x^2 \sin x\,dx ∫ x 2 sin x d x
Apply integration by parts twice.
First: u = x 2 u = x^2 u = x 2 , d v = sin x d x dv = \sin x\,dx d v = sin x d x , so d u = 2 x d x du = 2x\,dx d u = 2 x d x , v = − cos x v = -\cos x v = − cos x .
∫ x 2 sin x d x = − x 2 cos x + 2 ∫ x cos x d x \int x^2 \sin x\,dx = -x^2 \cos x + 2\int x \cos x\,dx ∫ x 2 sin x d x = − x 2 cos x + 2 ∫ x cos x d x Second: u = x u = x u = x , d v = cos x d x dv = \cos x\,dx d v = cos x d x , so d u = d x du = dx d u = d x , v = sin x v = \sin x v = sin x .
\begin`\{aligned}`
\int x^2 \sin x\,dx &= -x^2 \cos x + 2\left(x\sin x - \int \sin x\,dx\right) \\[6pt]
&= -x^2 \cos x + 2x\sin x + 2\cos x + C
\end`\{aligned}`
3.3 Partial Fractions
When the integrand is a rational function P ( x ) Q ( x ) \dfrac{P(x)}{Q(x)} Q ( x ) P ( x ) where deg P < deg Q \deg P < \deg Q deg P < deg Q and Q Q Q
factors into linear or irreducible quadratic factors, partial fraction decomposition converts the
integrand into a sum of simpler fractions.
Decomposition rules:
Factor in Q ( x ) Q(x) Q ( x ) Term in decomposition ( a x + b ) (ax + b) ( a x + b ) A a x + b \dfrac{A}{ax + b} a x + b A ( a x + b ) k (ax + b)^k ( a x + b ) k A 1 a x + b + A 2 ( a x + b ) 2 + ⋯ + A k ( a x + b ) k \dfrac{A_1}{ax + b} + \dfrac{A_2}{(ax+b)^2} + \cdots + \dfrac{A_k}{(ax+b)^k} a x + b A 1 + ( a x + b ) 2 A 2 + ⋯ + ( a x + b ) k A k a x 2 + b x + c ax^2 + bx + c a x 2 + b x + c (irreducible)A x + B a x 2 + b x + c \dfrac{Ax + B}{ax^2 + bx + c} a x 2 + b x + c A x + B
Details
Expand
Find ∫ 5 x + 1 ( x + 1 ) ( x − 2 ) d x \int \frac{5x + 1}{(x+1)(x-2)}\,dx ∫ ( x + 1 ) ( x − 2 ) 5 x + 1 d x
Decompose: 5 x + 1 ( x + 1 ) ( x − 2 ) = A x + 1 + B x − 2 \dfrac{5x + 1}{(x+1)(x-2)} = \dfrac{A}{x+1} + \dfrac{B}{x-2} ( x + 1 ) ( x − 2 ) 5 x + 1 = x + 1 A + x − 2 B
5 x + 1 = A ( x − 2 ) + B ( x + 1 ) 5x + 1 = A(x - 2) + B(x + 1) 5 x + 1 = A ( x − 2 ) + B ( x + 1 ) Setting x = − 1 x = -1 x = − 1 : − 5 + 1 = A ( − 3 ) ⟹ A = 4 3 -5 + 1 = A(-3) \implies A = \frac{4}{3} − 5 + 1 = A ( − 3 ) ⟹ A = 3 4
Setting x = 2 x = 2 x = 2 : 10 + 1 = B ( 3 ) ⟹ B = 11 3 10 + 1 = B(3) \implies B = \frac{11}{3} 10 + 1 = B ( 3 ) ⟹ B = 3 11
∫ 5 x + 1 ( x + 1 ) ( x − 2 ) d x = 4 3 ln ∣ x + 1 ∣ + 11 3 ln ∣ x − 2 ∣ + C \int \frac{5x + 1}{(x+1)(x-2)}\,dx = \frac{4}{3}\ln|x+1| + \frac{11}{3}\ln|x-2| + C ∫ ( x + 1 ) ( x − 2 ) 5 x + 1 d x = 3 4 ln ∣ x + 1∣ + 3 11 ln ∣ x − 2∣ + C
3.4 Trigonometric Integrals
Several standard techniques apply to integrals involving trigonometric functions.
Pythagorean identities for conversion:
sin 2 x = 1 − cos 2 x 2 , cos 2 x = 1 + cos 2 x 2 \sin^2 x = \frac{1 - \cos 2x}{2}, \qquad \cos^2 x = \frac{1 + \cos 2x}{2} sin 2 x = 2 1 − cos 2 x , cos 2 x = 2 1 + cos 2 x
These are used to reduce the power of trigonometric functions in integrands.
Products to sums:
sin A cos B = 1 2 [ sin ( A + B ) + sin ( A − B ) ] \sin A \cos B = \frac{1}{2}[\sin(A+B) + \sin(A-B)] sin A cos B = 2 1 [ sin ( A + B ) + sin ( A − B )]
cos A cos B = 1 2 [ cos ( A − B ) + cos ( A + B ) ] \cos A \cos B = \frac{1}{2}[\cos(A-B) + \cos(A+B)] cos A cos B = 2 1 [ cos ( A − B ) + cos ( A + B )]
sin A sin B = 1 2 [ cos ( A − B ) − cos ( A + B ) ] \sin A \sin B = \frac{1}{2}[\cos(A-B) - \cos(A+B)] sin A sin B = 2 1 [ cos ( A − B ) − cos ( A + B )]
Using substitution with trigonometric derivatives: Recall that d d x ( sin x ) = cos x \dfrac{d}{dx}(\sin x) = \cos x d x d ( sin x ) = cos x
and d d x ( cos x ) = − sin x \dfrac{d}{dx}(\cos x) = -\sin x d x d ( cos x ) = − sin x . Many trigonometric integrals yield to u u u -substitution when
the derivative of one trigonometric factor is present.
Integrals of the form ∫ tan n x d x \int \tan^n x\,dx ∫ tan n x d x : Rewrite in terms of sec 2 x \sec^2 x sec 2 x and use
d d x ( tan x ) = sec 2 x \dfrac{d}{dx}(\tan x) = \sec^2 x d x d ( tan x ) = sec 2 x .
Details
Expand
Find ∫ sin 2 x d x \int \sin^2 x\,dx ∫ sin 2 x d x
∫ sin 2 x d x = ∫ 1 − cos 2 x 2 d x = x 2 − sin 2 x 4 + C \int \sin^2 x\,dx = \int \frac{1 - \cos 2x}{2}\,dx = \frac{x}{2} - \frac{\sin 2x}{4} + C ∫ sin 2 x d x = ∫ 2 1 − cos 2 x d x = 2 x − 4 sin 2 x + C Find ∫ sin 3 x d x \int \sin^3 x\,dx ∫ sin 3 x d x
\begin`\{aligned}`
\int \sin^3 x\,dx &= \int \sin x (1 - \cos^2 x)\,dx \\[6pt]
&= \int \sin x\,dx - \int \sin x \cos^2 x\,dx \\[6pt]
&= -\cos x + \frac{\cos^3 x}{3} + C
\end`\{aligned}` (using u = cos x u = \cos x u = cos x , d u = − sin x d x du = -\sin x\,dx d u = − sin x d x for the second integral)
4. Applications of Integration
4.1 Area Between Two Curves
Given two continuous functions f f f and g g g with f ( x ) ≥ g ( x ) f(x) \geq g(x) f ( x ) ≥ g ( x ) on [ a , b ] [a, b] [ a , b ] , the area between the
curves is:
A = ∫ a b [ f ( x ) − g ( x ) ] d x A = \int_a^b [f(x) - g(x)]\,dx A = ∫ a b [ f ( x ) − g ( x )] d x
If the curves intersect, find the points of intersection and split the integral accordingly so that
the integrand ∣ f ( x ) − g ( x ) ∣ |f(x) - g(x)| ∣ f ( x ) − g ( x ) ∣ is always non-negative.
Horizontal strips: When integrating with respect to y y y , the formula becomes:
A = ∫ c d [ f ( y ) − g ( y ) ] d y A = \int_c^d [f(y) - g(y)]\,dy A = ∫ c d [ f ( y ) − g ( y )] d y
where the curves are expressed as x = f ( y ) x = f(y) x = f ( y ) and x = g ( y ) x = g(y) x = g ( y ) .
Details
Expand
Find the area between y = x 2 y = x^2 y = x 2 and y = 2 x y = 2x y = 2 x .
Intersection: x 2 = 2 x ⟹ x = 0 x^2 = 2x \implies x = 0 x 2 = 2 x ⟹ x = 0 or x = 2 x = 2 x = 2 . On [ 0 , 2 ] [0, 2] [ 0 , 2 ] , 2 x ≥ x 2 2x \geq x^2 2 x ≥ x 2 .
A = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − x 3 3 ] 0 2 = 4 − 8 3 = 4 3 A = \int_0^2 (2x - x^2)\,dx = \left[x^2 - \frac{x^3}{3}\right]_0^2 = 4 - \frac{8}{3} = \frac{4}{3} A = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − 3 x 3 ] 0 2 = 4 − 3 8 = 3 4
4.2 Volumes of Revolution
When a region bounded by y = f ( x ) y = f(x) y = f ( x ) , the x x x -axis, and the lines x = a x = a x = a , x = b x = b x = b is revolved about
the x x x -axis, the volume of the solid of revolution is:
V = π ∫ a b [ f ( x ) ] 2 d x V = \pi \int_a^b [f(x)]^2\,dx V = π ∫ a b [ f ( x ) ] 2 d x
Revolution about the y y y -axis:
V = π ∫ c d [ g ( y ) ] 2 d y V = \pi \int_c^d [g(y)]^2\,dy V = π ∫ c d [ g ( y ) ] 2 d y
where x = g ( y ) x = g(y) x = g ( y ) .
Revolution about a horizontal line y = k y = k y = k :
V = π ∫ a b [ f ( x ) − k ] 2 d x V = \pi \int_a^b [f(x) - k]^2\,dx V = π ∫ a b [ f ( x ) − k ] 2 d x
Washer method (volume between two surfaces):
V = π ∫ a b ( [ f ( x ) ] 2 − [ g ( x ) ] 2 ) d x V = \pi \int_a^b \left([f(x)]^2 - [g(x)]^2\right)\,dx V = π ∫ a b ( [ f ( x ) ] 2 − [ g ( x ) ] 2 ) d x
where f ( x ) ≥ g ( x ) ≥ 0 f(x) \geq g(x) \geq 0 f ( x ) ≥ g ( x ) ≥ 0 on [ a , b ] [a, b] [ a , b ] .
Details
Expand
Find the volume generated by revolving y = x y = \sqrt{x} y = x about the x x x -axis from x = 0 x = 0 x = 0 to
x = 4 x = 4 x = 4 .
\begin`\{aligned}`
V &= \pi \int_0^4 (\sqrt{x})^2\,dx = \pi \int_0^4 x\,dx \\[6pt]
&= \pi \left[\frac{x^2}{2}\right]_0^4 = 8\pi
\end`\{aligned}`
4.3 Kinematics
Integration connects the kinematic quantities:
v ( t ) = ∫ a ( t ) d t + v 0 v(t) = \int a(t)\,dt + v_0 v ( t ) = ∫ a ( t ) d t + v 0
s ( t ) = ∫ v ( t ) d t + s 0 s(t) = \int v(t)\,dt + s_0 s ( t ) = ∫ v ( t ) d t + s 0
where a ( t ) a(t) a ( t ) is acceleration, v ( t ) v(t) v ( t ) is velocity, s ( t ) s(t) s ( t ) is displacement, and v 0 v_0 v 0 , s 0 s_0 s 0 are
initial conditions.
Key relationships:
The displacement over a time interval [ t 1 , t 2 ] [t_1, t_2] [ t 1 , t 2 ] is
∫ t 1 t 2 v ( t ) d t \displaystyle\int_{t_1}^{t_2} v(t)\,dt ∫ t 1 t 2 v ( t ) d t .
The total distance travelled is ∫ t 1 t 2 ∣ v ( t ) ∣ d t \displaystyle\int_{t_1}^{t_2} |v(t)|\,dt ∫ t 1 t 2 ∣ v ( t ) ∣ d t .
The velocity is the derivative of displacement: v = d s d t v = \dfrac{ds}{dt} v = d t d s .
The acceleration is the derivative of velocity: a = d v d t a = \dfrac{dv}{dt} a = d t d v .
Details
Expand
A particle moves with velocity v ( t ) = 6 t 2 − 4 t v(t) = 6t^2 - 4t v ( t ) = 6 t 2 − 4 t m/s for t ≥ 0 t \geq 0 t ≥ 0 . Find the displacement and
total distance in the first 3 seconds.
Displacement:
∫ 0 3 ( 6 t 2 − 4 t ) d t = [ 2 t 3 − 2 t 2 ] 0 3 = 54 − 18 = 36 m \int_0^3 (6t^2 - 4t)\,dt = \left[2t^3 - 2t^2\right]_0^3 = 54 - 18 = 36 \mathrm{ m} ∫ 0 3 ( 6 t 2 − 4 t ) d t = [ 2 t 3 − 2 t 2 ] 0 3 = 54 − 18 = 36 m Total distance: find when v ( t ) = 0 v(t) = 0 v ( t ) = 0 : 6 t 2 − 4 t = 0 ⟹ t = 0 6t^2 - 4t = 0 \implies t = 0 6 t 2 − 4 t = 0 ⟹ t = 0 or t = 2 3 t = \frac{2}{3} t = 3 2 .
\begin`\{aligned}`
\mathrm{Distance} &= \int_0^{2/3} |6t^2 - 4t|\,dt + \int_{2/3}^3 |6t^2 - 4t|\,dt \\[6pt]
&= \int_0^{2/3} (4t - 6t^2)\,dt + \int_{2/3}^3 (6t^2 - 4t)\,dt \\[6pt]
&= \left[2t^2 - 2t^3\right]_0^{2/3} + \left[2t^3 - 2t^2\right]_{2/3}^3 \\[6pt]
&= \frac{8}{27} + \left(36 - \left(-\frac{8}{27}\right)\right) = \frac{8}{27} + 36 + \frac{8}{27} = \frac{988}{27} \approx 36.6 \mathrm{ m}
\end`\{aligned}`
5. Properties of Definite Integrals
These properties follow from the definition of the definite integral and are essential for
simplifying computations.
Linearity
∫ a b [ k f ( x ) + l g ( x ) ] d x = k ∫ a b f ( x ) d x + l ∫ a b g ( x ) d x \int_a^b [k f(x) + l g(x)]\,dx = k\int_a^b f(x)\,dx + l\int_a^b g(x)\,dx ∫ a b [ k f ( x ) + l g ( x )] d x = k ∫ a b f ( x ) d x + l ∫ a b g ( x ) d x
for constants k , l ∈ ′ { ′ R ′ } ′ k, l \in \mathbb{'\{'}R{'\}'} k , l ∈ ′ { ′ R ′ } ′ .
Reversal of Limits
∫ a b f ( x ) d x = − ∫ b a f ( x ) d x \int_a^b f(x)\,dx = -\int_b^a f(x)\,dx ∫ a b f ( x ) d x = − ∫ b a f ( x ) d x
Interval of Zero Length
∫ a a f ( x ) d x = 0 \int_a^a f(x)\,dx = 0 ∫ a a f ( x ) d x = 0
Additivity Over Intervals
∫ a b f ( x ) d x = ∫ a c f ( x ) d x + ∫ c b f ( x ) d x \int_a^b f(x)\,dx = \int_a^c f(x)\,dx + \int_c^b f(x)\,dx ∫ a b f ( x ) d x = ∫ a c f ( x ) d x + ∫ c b f ( x ) d x
for any c ∈ [ a , b ] c \in [a, b] c ∈ [ a , b ] .
Comparison Properties
If f ( x ) ≥ 0 f(x) \geq 0 f ( x ) ≥ 0 for all x ∈ [ a , b ] x \in [a, b] x ∈ [ a , b ] , then ∫ a b f ( x ) d x ≥ 0 \displaystyle\int_a^b f(x)\,dx \geq 0 ∫ a b f ( x ) d x ≥ 0 .
If f ( x ) ≥ g ( x ) f(x) \geq g(x) f ( x ) ≥ g ( x ) for all x ∈ [ a , b ] x \in [a, b] x ∈ [ a , b ] , then
∫ a b f ( x ) d x ≥ ∫ a b g ( x ) d x \displaystyle\int_a^b f(x)\,dx \geq \int_a^b g(x)\,dx ∫ a b f ( x ) d x ≥ ∫ a b g ( x ) d x .
Bounds on the Integral
If m ≤ f ( x ) ≤ M m \leq f(x) \leq M m ≤ f ( x ) ≤ M for all x ∈ [ a , b ] x \in [a, b] x ∈ [ a , b ] , then:
m ( b − a ) ≤ ∫ a b f ( x ) d x ≤ M ( b − a ) m(b - a) \leq \int_a^b f(x)\,dx \leq M(b - a) m ( b − a ) ≤ ∫ a b f ( x ) d x ≤ M ( b − a )
Details
Expand
Given ∫ 1 3 f ( x ) d x = 5 \int_1^3 f(x)\,dx = 5 ∫ 1 3 f ( x ) d x = 5 and ∫ 1 3 g ( x ) d x = − 2 \int_1^3 g(x)\,dx = -2 ∫ 1 3 g ( x ) d x = − 2 , find ∫ 3 1 [ 3 f ( x ) − 2 g ( x ) ] d x \int_3^1 [3f(x) - 2g(x)]\,dx ∫ 3 1 [ 3 f ( x ) − 2 g ( x )] d x .
\begin`\{aligned}`
\int_3^1 [3f(x) - 2g(x)]\,dx &= -\int_1^3 [3f(x) - 2g(x)]\,dx \\[6pt]
&= -\left(3 \cdot 5 - 2 \cdot (-2)\right) = -(15 + 4) = -19
\end`\{aligned}`
6. Improper Integrals (HL)
Improper integrals extend the concept of definite integration to cases where the interval of
integration is unbounded or the integrand has a vertical asymptote within (or at an endpoint of) the
interval of integration.
Type 1: Infinite Limits of Integration
∫ a ∞ f ( x ) d x = lim t → ∞ ∫ a t f ( x ) d x \int_a^{\infty} f(x)\,dx = \lim_{t \to \infty} \int_a^t f(x)\,dx ∫ a ∞ f ( x ) d x = t → ∞ lim ∫ a t f ( x ) d x
∫ − ∞ b f ( x ) d x = lim t → − ∞ ∫ t b f ( x ) d x \int_{-\infty}^b f(x)\,dx = \lim_{t \to -\infty} \int_t^b f(x)\,dx ∫ − ∞ b f ( x ) d x = t → − ∞ lim ∫ t b f ( x ) d x
∫ − ∞ ∞ f ( x ) d x = ∫ − ∞ c f ( x ) d x + ∫ c ∞ f ( x ) d x \int_{-\infty}^{\infty} f(x)\,dx = \int_{-\infty}^c f(x)\,dx + \int_c^{\infty} f(x)\,dx ∫ − ∞ ∞ f ( x ) d x = ∫ − ∞ c f ( x ) d x + ∫ c ∞ f ( x ) d x
Both limits must converge independently for the integral to converge.
Type 2: Integrands with Vertical Asymptotes
If f f f has a vertical asymptote at x = a x = a x = a :
∫ a b f ( x ) d x = lim t → a + ∫ t b f ( x ) d x \int_a^b f(x)\,dx = \lim_{t \to a^+} \int_t^b f(x)\,dx ∫ a b f ( x ) d x = t → a + lim ∫ t b f ( x ) d x
If f f f has a vertical asymptote at x = b x = b x = b :
∫ a b f ( x ) d x = lim t → b − ∫ a t f ( x ) d x \int_a^b f(x)\,dx = \lim_{t \to b^-} \int_a^t f(x)\,dx ∫ a b f ( x ) d x = t → b − lim ∫ a t f ( x ) d x
If f f f has a vertical asymptote at an interior point x = c ∈ ( a , b ) x = c \in (a, b) x = c ∈ ( a , b ) :
∫ a b f ( x ) d x = lim t → c − ∫ a t f ( x ) d x + lim t → c + ∫ t b f ( x ) d x \int_a^b f(x)\,dx = \lim_{t \to c^-} \int_a^t f(x)\,dx + \lim_{t \to c^+} \int_t^b f(x)\,dx ∫ a b f ( x ) d x = t → c − lim ∫ a t f ( x ) d x + t → c + lim ∫ t b f ( x ) d x
Convergence and Divergence
An improper integral converges if the corresponding limit exists and is finite. It diverges
otherwise.
p p p -test for convergence: The integral ∫ 1 ∞ 1 x p d x \displaystyle\int_1^{\infty} \frac{1}{x^p}\,dx ∫ 1 ∞ x p 1 d x
converges if and only if p > 1 p > 1 p > 1 , in which case:
∫ 1 ∞ 1 x p d x = 1 p − 1 \int_1^{\infty} \frac{1}{x^p}\,dx = \frac{1}{p - 1} ∫ 1 ∞ x p 1 d x = p − 1 1
Similarly, ∫ 0 1 1 x p d x \displaystyle\int_0^1 \frac{1}{x^p}\,dx ∫ 0 1 x p 1 d x converges if and only if p < 1 p < 1 p < 1 .
Comparison test: If 0 ≤ f ( x ) ≤ g ( x ) 0 \leq f(x) \leq g(x) 0 ≤ f ( x ) ≤ g ( x ) for all x ≥ a x \geq a x ≥ a , and ∫ a ∞ g ( x ) d x \int_a^{\infty} g(x)\,dx ∫ a ∞ g ( x ) d x
converges, then ∫ a ∞ f ( x ) d x \int_a^{\infty} f(x)\,dx ∫ a ∞ f ( x ) d x also converges. Conversely, if ∫ a ∞ f ( x ) d x \int_a^{\infty} f(x)\,dx ∫ a ∞ f ( x ) d x
diverges, then ∫ a ∞ g ( x ) d x \int_a^{\infty} g(x)\,dx ∫ a ∞ g ( x ) d x also diverges.
Details
Expand
Determine whether ∫ 1 ∞ 1 x 2 d x \displaystyle\int_1^{\infty} \frac{1}{x^2}\,dx ∫ 1 ∞ x 2 1 d x converges.
\begin`\{aligned}`
\int_1^{\infty} \frac{1}{x^2}\,dx &= \lim_{t \to \infty} \int_1^t x^{-2}\,dx = \lim_{t \to \infty} \left[-\frac{1}{x}\right]_1^t \\[6pt]
&= \lim_{t \to \infty} \left(-\frac{1}{t} + 1\right) = 1
\end`\{aligned}` The integral converges to 1 1 1 . (Consistent with the p p p -test: p = 2 > 1 p = 2 > 1 p = 2 > 1 .)
Determine whether ∫ 0 1 1 x d x \displaystyle\int_0^1 \frac{1}{\sqrt{x}}\,dx ∫ 0 1 x 1 d x converges.
\begin`\{aligned}`
\int_0^1 \frac{1}{\sqrt{x}}\,dx &= \lim_{t \to 0^+} \int_t^1 x^{-1/2}\,dx = \lim_{t \to 0^+} \Big[2\sqrt{x}\Big]_t^1 \\[6pt]
&= \lim_{t \to 0^+} (2 - 2\sqrt{t}) = 2
\end`\{aligned}` The integral converges to 2 2 2 . (Consistent with the p p p -test: p = 1 2 < 1 p = \frac{1}{2} < 1 p = 2 1 < 1 .)
7. Practice Problems
Details
Find ∫ x 3 + 2 x x 2 + 1 d x \int \frac{x^3 + 2x}{\sqrt{x^2 + 1}}\,dx ∫ x 2 + 1 x 3 + 2 x d x
Let
u = x 2 + 1 u = x^2 + 1 u = x 2 + 1 ,
d u = 2 x d x du = 2x\,dx d u = 2 x d x . Note that
x 3 + 2 x = x ( x 2 + 1 ) + x = x u + u − 1 2 + 1 2 x^3 + 2x = x(x^2 + 1) + x = xu + \frac{u - 1}{2} + \frac{1}{2} x 3 + 2 x = x ( x 2 + 1 ) + x = xu + 2 u − 1 + 2 1 .
Alternatively, split:
x 3 + 2 x x 2 + 1 = x ( x 2 + 1 ) x 2 + 1 + x x 2 + 1 = x x 2 + 1 + x x 2 + 1 \dfrac{x^3 + 2x}{\sqrt{x^2 + 1}} = \dfrac{x(x^2 + 1)}{\sqrt{x^2 + 1}} + \dfrac{x}{\sqrt{x^2 + 1}} = x\sqrt{x^2 + 1} + \dfrac{x}{\sqrt{x^2 + 1}} x 2 + 1 x 3 + 2 x = x 2 + 1 x ( x 2 + 1 ) + x 2 + 1 x = x x 2 + 1 + x 2 + 1 x .
\begin`\{aligned}`
\int x\sqrt{x^2 + 1}\,dx &= \frac{1}{3}(x^2 + 1)^{3/2} + C_1 \\[6pt]
\int \frac{x}{\sqrt{x^2 + 1}}\,dx &= \sqrt{x^2 + 1} + C_2
\end`\{aligned}` ∫ x 3 + 2 x x 2 + 1 d x = 1 3 ( x 2 + 1 ) 3 / 2 + x 2 + 1 + C \int \frac{x^3 + 2x}{\sqrt{x^2 + 1}}\,dx = \frac{1}{3}(x^2 + 1)^{3/2} + \sqrt{x^2 + 1} + C ∫ x 2 + 1 x 3 + 2 x d x = 3 1 ( x 2 + 1 ) 3/2 + x 2 + 1 + C
Details
Evaluate ∫ 0 π / 2 x sin x d x \int_0^{\pi/2} x\sin x\,dx ∫ 0 π /2 x sin x d x
Integration by parts:
u = x u = x u = x ,
d v = sin x d x dv = \sin x\,dx d v = sin x d x , so
d u = d x du = dx d u = d x ,
v = − cos x v = -\cos x v = − cos x .
\begin`\{aligned}`
\int_0^{\pi/2} x\sin x\,dx &= \Big[-x\cos x\Big]_0^{\pi/2} + \int_0^{\pi/2} \cos x\,dx \\[6pt]
&= (0 - 0) + \Big[\sin x\Big]_0^{\pi/2} = 1
\end`\{aligned}`
Details
Find the area enclosed by y = x 3 y = x^3 y = x 3 and y = x y = x y = x .
Intersection points:
x 3 = x ⟹ x ( x 2 − 1 ) = 0 ⟹ x = − 1 , 0 , 1 x^3 = x \implies x(x^2 - 1) = 0 \implies x = -1, 0, 1 x 3 = x ⟹ x ( x 2 − 1 ) = 0 ⟹ x = − 1 , 0 , 1 .
On [ − 1 , 0 ] [-1, 0] [ − 1 , 0 ] : x 3 ≥ x x^3 \geq x x 3 ≥ x . On [ 0 , 1 ] [0, 1] [ 0 , 1 ] : x ≥ x 3 x \geq x^3 x ≥ x 3 .
\begin`\{aligned}`
A &= \int_{-1}^0 (x^3 - x)\,dx + \int_0^1 (x - x^3)\,dx \\[6pt]
&= \left[\frac{x^4}{4} - \frac{x^2}{2}\right]_{-1}^0 + \left[\frac{x^2}{2} - \frac{x^4}{4}\right]_0^1 \\[6pt]
&= \left(0 - \frac{1}{4} + \frac{1}{2}\right) + \left(\frac{1}{2} - \frac{1}{4}\right) = \frac{1}{4} + \frac{1}{4} = \frac{1}{2}
\end`\{aligned}`
Details
Find the volume of revolution when the region bounded by y = ln x y = \ln x y = ln x , x = e x = e x = e , and the x x x -axis is rotated about the x x x -axis.
The curve
y = ln x y = \ln x y = ln x meets the
x x x -axis at
x = 1 x = 1 x = 1 .
\begin`\{aligned}`
V &= \pi \int_1^e (\ln x)^2\,dx
\end`\{aligned}` Integration by parts with u = ( ln x ) 2 u = (\ln x)^2 u = ( ln x ) 2 , d v = d x dv = dx d v = d x : d u = 2 ln x x d x du = \dfrac{2\ln x}{x}\,dx d u = x 2 ln x d x , v = x v = x v = x .
\begin`\{aligned}`
\int (\ln x)^2\,dx &= x(\ln x)^2 - 2\int \ln x\,dx
\end`\{aligned}` Apply parts again for ∫ ln x d x \int \ln x\,dx ∫ ln x d x : u = ln x u = \ln x u = ln x , d v = d x dv = dx d v = d x , so ∫ ln x d x = x ln x − x \int \ln x\,dx = x\ln x - x ∫ ln x d x = x ln x − x .
\begin`\{aligned}`
\int (\ln x)^2\,dx &= x(\ln x)^2 - 2(x\ln x - x) + C \\[6pt]
&= x(\ln x)^2 - 2x\ln x + 2x + C
\end`\{aligned}` Evaluating from 1 1 1 to e e e :
\begin`\{aligned}`
\Big[x(\ln x)^2 - 2x\ln x + 2x\Big]_1^e &= (e - 2e + 2e) - (0 - 0 + 2) = e - 2
\end`\{aligned}` V = π ( e − 2 ) V = \pi(e - 2) V = π ( e − 2 )
Use partial fractions to find ∫ 3 x + 7 ( x + 2 ) ( x − 1 ) d x \int \frac{3x + 7}{(x + 2)(x - 1)}\,dx ∫ ( x + 2 ) ( x − 1 ) 3 x + 7 d x . 3 x + 7 ( x + 2 ) ( x − 1 ) = A x + 2 + B x − 1 \frac{3x + 7}{(x+2)(x-1)} = \frac{A}{x+2} + \frac{B}{x-1} ( x + 2 ) ( x − 1 ) 3 x + 7 = x + 2 A + x − 1 B 3 x + 7 = A ( x − 1 ) + B ( x + 2 ) 3x + 7 = A(x - 1) + B(x + 2) 3 x + 7 = A ( x − 1 ) + B ( x + 2 ) x = 1 x = 1 x = 1 : 10 = 3 B ⟹ B = 10 3 10 = 3B \implies B = \dfrac{10}{3} 10 = 3 B ⟹ B = 3 10
x = − 2 x = -2 x = − 2 : 1 = − 3 A ⟹ A = − 1 3 1 = -3A \implies A = -\dfrac{1}{3} 1 = − 3 A ⟹ A = − 3 1
∫ 3 x + 7 ( x + 2 ) ( x − 1 ) d x = − 1 3 ln ∣ x + 2 ∣ + 10 3 ln ∣ x − 1 ∣ + C \int \frac{3x + 7}{(x+2)(x-1)}\,dx = -\frac{1}{3}\ln|x+2| + \frac{10}{3}\ln|x-1| + C ∫ ( x + 2 ) ( x − 1 ) 3 x + 7 d x = − 3 1 ln ∣ x + 2∣ + 3 10 ln ∣ x − 1∣ + C
A particle moves with acceleration a ( t ) = 6 t − 2 a(t) = 6t - 2 a ( t ) = 6 t − 2 m/s2 ^2 2 . Initially, v ( 0 ) = 4 v(0) = 4 v ( 0 ) = 4 m/s and s ( 0 ) = 0 s(0) = 0 s ( 0 ) = 0 m. Find s ( t ) s(t) s ( t ) and the displacement after 3 seconds. v ( t ) = ∫ ( 6 t − 2 ) d t + 4 = 3 t 2 − 2 t + 4 v(t) = \int (6t - 2)\,dt + 4 = 3t^2 - 2t + 4 v ( t ) = ∫ ( 6 t − 2 ) d t + 4 = 3 t 2 − 2 t + 4 s ( t ) = ∫ ( 3 t 2 − 2 t + 4 ) d t + 0 = t 3 − t 2 + 4 t s(t) = \int (3t^2 - 2t + 4)\,dt + 0 = t^3 - t^2 + 4t s ( t ) = ∫ ( 3 t 2 − 2 t + 4 ) d t + 0 = t 3 − t 2 + 4 t Displacement at t = 3 t = 3 t = 3 :
s ( 3 ) = 27 − 9 + 12 = 30 m s(3) = 27 - 9 + 12 = 30 \mathrm{ m} s ( 3 ) = 27 − 9 + 12 = 30 m
Details
Determine whether ∫ 2 ∞ 1 x ( ln x ) 2 d x \displaystyle\int_2^{\infty} \frac{1}{x(\ln x)^2}\,dx ∫ 2 ∞ x ( ln x ) 2 1 d x converges, and evaluate if it does.
Let
u = ln x u = \ln x u = ln x ,
d u = 1 x d x du = \dfrac{1}{x}\,dx d u = x 1 d x . When
x = 2 x = 2 x = 2 ,
u = ln 2 u = \ln 2 u = ln 2 ; when
x → ∞ x \to \infty x → ∞ ,
u → ∞ u \to \infty u → ∞ .
\begin`\{aligned}`
\int_2^{\infty} \frac{1}{x(\ln x)^2}\,dx &= \int_{\ln 2}^{\infty} \frac{1}{u^2}\,du = \lim_{t \to \infty} \int_{\ln 2}^t u^{-2}\,du \\[6pt]
&= \lim_{t \to \infty} \left[-\frac{1}{u}\right]_{\ln 2}^t = \lim_{t \to \infty} \left(-\frac{1}{t} + \frac{1}{\ln 2}\right) = \frac{1}{\ln 2}
\end`\{aligned}` The integral converges to 1 ln 2 \dfrac{1}{\ln 2} ln 2 1 .
Details
Evaluate ∫ x 2 x 2 − 1 d x \int \frac{x^2}{x^2 - 1}\,dx ∫ x 2 − 1 x 2 d x using polynomial long division and partial fractions.
Since
deg ( n u m e r a t o r ) = deg ( d e n o m i n a t o r ) \deg(\mathrm{numerator}) = \deg(\mathrm{denominator}) deg ( numerator ) = deg ( denominator ) , perform long division first:
x 2 x 2 − 1 = 1 + 1 x 2 − 1 = 1 + 1 ( x − 1 ) ( x + 1 ) \frac{x^2}{x^2 - 1} = 1 + \frac{1}{x^2 - 1} = 1 + \frac{1}{(x-1)(x+1)} x 2 − 1 x 2 = 1 + x 2 − 1 1 = 1 + ( x − 1 ) ( x + 1 ) 1 Partial fractions: 1 ( x − 1 ) ( x + 1 ) = A x − 1 + B x + 1 \dfrac{1}{(x-1)(x+1)} = \dfrac{A}{x-1} + \dfrac{B}{x+1} ( x − 1 ) ( x + 1 ) 1 = x − 1 A + x + 1 B
1 = A ( x + 1 ) + B ( x − 1 ) 1 = A(x+1) + B(x-1) 1 = A ( x + 1 ) + B ( x − 1 )
x = 1 x = 1 x = 1 : A = 1 2 A = \dfrac{1}{2} A = 2 1 , x = − 1 x = -1 x = − 1 : B = − 1 2 B = -\dfrac{1}{2} B = − 2 1
\begin`\{aligned}`
\int \frac{x^2}{x^2 - 1}\,dx &= \int \left(1 + \frac{1}{2(x-1)} - \frac{1}{2(x+1)}\right)\,dx \\[6pt]
&= x + \frac{1}{2}\ln|x-1| - \frac{1}{2}\ln|x+1| + C
\end`\{aligned}`
Details
Evaluate ∫ 0 1 e x 1 + e x d x \int_0^1 \frac{e^x}{1 + e^x}\,dx ∫ 0 1 1 + e x e x d x .
Let
u = 1 + e x u = 1 + e^x u = 1 + e x ,
d u = e x d x du = e^x\,dx d u = e x d x . When
x = 0 x = 0 x = 0 ,
u = 2 u = 2 u = 2 ; when
x = 1 x = 1 x = 1 ,
u = 1 + e u = 1 + e u = 1 + e .
∫ 0 1 e x 1 + e x d x = ∫ 2 1 + e 1 u d u = [ ln u ] 2 1 + e = ln ( 1 + e ) − ln 2 \int_0^1 \frac{e^x}{1 + e^x}\,dx = \int_2^{1+e} \frac{1}{u}\,du = \Big[\ln u\Big]_2^{1+e} = \ln(1 + e) - \ln 2 ∫ 0 1 1 + e x e x d x = ∫ 2 1 + e u 1 d u = [ ln u ] 2 1 + e = ln ( 1 + e ) − ln 2
Details
Find ∫ e x cos x d x \int e^x \cos x\,dx ∫ e x cos x d x using integration by parts twice.
Let
I = ∫ e x cos x d x I = \displaystyle\int e^x \cos x\,dx I = ∫ e x cos x d x .
First application: u = e x u = e^x u = e x , d v = cos x d x dv = \cos x\,dx d v = cos x d x , so d u = e x d x du = e^x\,dx d u = e x d x , v = sin x v = \sin x v = sin x .
I = e x sin x − ∫ e x sin x d x I = e^x \sin x - \int e^x \sin x\,dx I = e x sin x − ∫ e x sin x d x Second application on ∫ e x sin x d x \int e^x \sin x\,dx ∫ e x sin x d x : u = e x u = e^x u = e x , d v = sin x d x dv = \sin x\,dx d v = sin x d x , so d u = e x d x du = e^x\,dx d u = e x d x ,
v = − cos x v = -\cos x v = − cos x .
∫ e x sin x d x = − e x cos x + ∫ e x cos x d x = − e x cos x + I \int e^x \sin x\,dx = -e^x \cos x + \int e^x \cos x\,dx = -e^x \cos x + I ∫ e x sin x d x = − e x cos x + ∫ e x cos x d x = − e x cos x + I Substituting back:
I = e x sin x − ( − e x cos x + I ) = e x sin x + e x cos x − I I = e^x \sin x - (-e^x \cos x + I) = e^x \sin x + e^x \cos x - I I = e x sin x − ( − e x cos x + I ) = e x sin x + e x cos x − I 2 I = e x ( sin x + cos x ) ⟹ I = e x ( sin x + cos x ) 2 + C 2I = e^x (\sin x + \cos x) \implies I = \frac{e^x (\sin x + \cos x)}{2} + C 2 I = e x ( sin x + cos x ) ⟹ I = 2 e x ( sin x + cos x ) + C
Cross-References
Differentiation -- Integration is the inverse operation of differentiation. See the
Number and Algebra notes for function fundamentals
including derivative rules that motivate integration techniques.
Functions -- Domain and range considerations determine when antiderivatives are valid. See
Number and Algebra for function fundamentals.
Complex Numbers -- The exponential form e i θ = cos θ + i sin θ e^{i\theta} = \cos\theta + i\sin\theta e i θ = cos θ + i sin θ provides an
elegant derivation of trigonometric integral results. See
Complex Numbers .
Logic -- Proof techniques (direct proof, contradiction) are used to justify properties of
integrals. See Logic .