Integral Calculus

Calculation Rules for undefined Integrals

a) Additivity A sum under the integral is integrated by the summands are integrated separately and then summed.

(f(x)+g(x))dx = f(x)dx+g(x)dx

b) Factor Rule A constant factor a can be pulled out of the integral.

af(x)dx = a f(x)dx

c) If F(u) is the antiderivative of f(u), then the following relationship holds for arbitrary constants a and b with a not equal to 0.

f(ax+b)dx = 1a F(ax+b)+C

d) If f(x) is differentiable and f(x) not equal to 0, then the following relationship applies.

f (x)f(x)dx = ln|f(x)|+C

e) Integration by parts Are the functions u(x) and v(x) are differentiable, then the following relationship holds.

(u(x)v(x))dx = u(x)v(x)-u(x)v(x)dx

f) Substitution If the function f(z) is continuous and z = g(x) is differentiable, then the following relationship holds.

(f(g(x))g(x))dx = f(z)dz

Basic Integrals

General

f(x)dx = f(x) dx = x

Power

xndx = xn+1n+1 (ax+b)ndx = (ax+b)n+1a(n+1) dxx = ln|x|

Exponential Functions

exdx = ex axdx = axlna

Trigonometric Functions

sinxdx = -cosx cosxdx = sinx tanxdx = -ln|cosx| dxcos2x = tanx dxsin2x = -cotx

Logarithmic Functions

lnxdx = xlnx-x (lnx)2dx = x(lnx)2-2xlnx+2x dxxlnx = ln(lnx)

Irrational Functions

ax+bdx = 23a(ax+b)3 dxax+b = 2ax+ba

Examples

Example: Linearity of the integral (Rule a and b)

(5x+2sin(x))dx

= 5xdx+2sin(x)dx

Due to the additivity of the summands can be integrated individually.

= 5xdx+2sin(x)dx

The constant factors are taken outside the integral.

= 52x2-2cos(x)+C

With the basic integrals, the solution follows.

Example: A function of a linear function (Rule c)

12x+3dx

f(ax+b) = 12x+3

The function under the integral is a function of a linear function.

F(u)=1udu=ln|u|+C

Formation of the primitive of f with the substitution u = ax + b.

= 12ln|2x+3|+C

Install in accordance with rule c yields the solution of the integral.

Example: f(x) in the denominator and the derivative of f(x) in the nominator (Rule d)

cos(x)sin(x)dx

ddxsin(x) = cos(x)

That means in the numerator is the derivative of the denominator.

= ln|sin(x)|+C

Install in accordance with rule d yields the solution of the integral.

Example: Integration by parts (Rule e)

x3ln(x)dx

x3dx = x44

Is the first factor v', then the integral of the first factor is v.

ddxln(x) = 1x

The derivative of the second factor is u'.

= x44ln(x)-14x3dx

Put in following rule e.

= x44ln(x)-14x44+C

With the integral of I the solution of the integral follows.

= x44(ln(x)-14)+C

This can be written also shorter by factoring out.

Example: Integration by substitution (Rule f)

xdxa2+x2

g(x) = a2+x2

Substitution of the denominator as a function g(x).

dgdx = xa2+x2 = xg

The derivative of g(x) by dx is the relationship according to the differentials.

xdx = gdg

Dissolved, the term can be used in the integral.

= gdgg = dg = g+C

Put in and integrated.

= g+C = a2+x2+C

Repatriation of substitution yields the solution.

Rules of calculation of definite integrals

The existence of the integrals in each case provided. There are a, b, c ∈ ℜ constants.

a) Interchange of the limits of integration.

abf(x)dx = -baf(x)dx

a1) Definition

aaf(x)dx = 0

b) Factor Rule A constant factor a can be pulled outside the integral.

abaf(x)dx = a abf(x)dx

c) Sum Rule A sum under the definite integral can be integrated by means of the summands.

abf(x)+g(x)dx = abf(x)dx+abg(x)dx

d) Decomposition of the definite integral in part integrals.

abf(x)dx = acf(x)dx+cbf(x)dx

e) Mean Value Theorem If f is integrable and we have m ≤ f ≤ M, then there exists at least one number μ with m ≤ μ ≤ M and we have the following relationship.

abf(x)dx = μ(b-a)

f) General Mean Value Theorem If f and g are integrable and we have m ≤ f ≤ M and g ≥ 0 either always or g ≤ 0, then there exists at least one number μ with m ≤ μ ≤ M and it works as follows.

abf(x)g(x)dx = μabg(x)dx

g) Second Mean Value Theorem If f is monotonic and bounded and g integrable, then there exists at least one number μ for which the following relationship is valid.

abf(x)g(x)dx = f(a)aμg(x)dx+f(b)μbg(x)dx

h) If a function f is continuous and differentiable, then applies

F(x) = axf(t)dt

with F(x) = f(x)

i) Main Theorem of the Differential and Integral Calculations. If the antiderivative F of f is known, then the definite integral of f is calculated as follows

abf(x)dx = F(b)-F(a)

j) Integration by parts Are the functions u (x) and v (x) is differentiable, then the following relationship holds.

ab(u(x)v(x))dx = [u(x)v(x)]ab-abu(x)v(x)dx

k) Substitution for definite integrals.

ab(f(g(x))g(x))dx = g(a)g(b)f(z)dz

Releated sites

Here is a list of of further useful sites:

Index Derivation rules Derivative calculator Matrix rules Determinant rules ODE first order General first order ODE ODE second order ODE-System 2x2 ODE-System 3x3 Exponential growth Logistic growth Bernoulli equation Riccati equation