- •Донецьк 2006
- •Integral calculus lecture no. 19. Primitive and indefinite integral
- •Point 1. Primitive
- •Properties of primitives
- •Point 2. Indefinite integral and its properties
- •Point 3. Integration by substitution (change of a variable)
- •Point 4. Integration by parts
- •Lecture no.20. Classes of integrable functions
- •Point 1. Rational functions (rational fractions)
- •Point 2. Trigonometric functions
- •Universal trigonometrical substitution
- •Other substitutions
- •Point 3. Irrational functions
- •Quadratic irrationalities. Trigonometric substitutions
- •Quadratic irrationalities (general case)
- •Indefinite integral: Basic Terminology
- •Lecture no. 21. Definite integral
- •Point 1. Problems leading to the concept ofa definite integral
- •Point 2. Definite integral
- •Point 3. Properties of a definite integral
- •I ntegration of inequalities
- •Point 4. Definite integral as a function of its upper variable limit
- •Point 5. Newton-leibniz formula
- •Point 6. Main methods of evaluation a definite integral Change of a variable (substitution method)
- •Integration by parts
- •Lecture no.22. Applications of definite integral
- •Point 1. Problem – solving schemes. Areas
- •Additional remarks about the areas of plane figures
- •Point 2. Arс length
- •Point 3. Volumes
- •Volume of a body with known areas of its parallel cross-sections
- •Volume of a body of rotation
- •Point 4. Economic applications
- •Lecture no. 23. Definite integral: additional questions
- •Point 1. Approximate integration
- •Rectangular Formulas
- •Trapezium Formula
- •Simpson10 formula (parabolic formula)
- •Point 2. Improper integrals
- •Improper integrals of the first kind
- •Improper integrals of the second kind
- •Convergence tests
- •Point 3. Euler г- function
- •Definite integral: Basic Terminology
- •Lecture no. 24. Double integral
- •Point 1. Double integral
- •Point 2. Evaluation of a double integral in cartesian coordinates
- •Point 3. Improper double integrals. Poisson formula
- •Point 4. Double integral in polar coordinates
- •Double integral: Basic Terminology
- •Differential equations lecture no.25. First and second order differential equations
- •Point 1. General notions
- •Point 2. Integrable types of the first order differential equations (of de - 1)
- •1. Separated de-1 (de-1 with separated variables)
- •2. Separable de-1 (de-1 with separable variables)
- •3. Homogeneous de-1
- •4. Linear de-1
- •5. Bernoulli de-1
- •Point 3. Order reducing second order differential equations
- •Lecture no.26. Second order linear differential equations
- •Point 1. General notions
- •Point 2. Linear dependence and independence
- •Point 3. Homogeneous equations Structure of the general solution of so lhde
- •So lhde with constant coefficients
- •Point 4. Nonhomogeneous equations Structure of the general solution of so lnde
- •Method of variation of arbitrary constants
- •Method of undetermined coefficients for so lnde with constant coefficients
- •Lecture no. 27. Systems of differential equations. Approximate integration of differential equations
- •Point 1. Normal systems of differential equations
- •Point 2. Approximate integration of differential equations Successive approximations method
- •Euler method
- •Differential equations: Basic Terminology
- •Bibliography textbooks
- •Problem books
- •Contents
Point 3. Order reducing second order differential equations
1. Second order differential equation resolved with respect to the higher derivative if the right member of the equation depends only on the independent variable
. ( 22 )
One finds the general solution of this equation by twice integration, namely
( 23 )
■
.■
Note 7. If it is a matter of Cauchy problem for the equation (22) with initial conditions
then it is well to integrate over an interval , namely
.
In this case we at once have
,
and the solution of Cauchy problem takes on the next form
.
Ex. 16. Solve the next Cauchy problem
Twice integrating we at first have the general solution of the differential equation,
.
Taking into account the initial conditions we find ,
.
Therefore the solution of Cauchy problem
.
2. Second order differential equation not containing explicitly the unknown function
( 24 )
reduces to the first order differential equation by introducing a new unknown function
. ( 25 )
So long as
,
the equation (24) passes to the next one
. ( 26 )
We’ve got the first order differential equation in .
Suppose that we’ve found the general solution of the equation (26) of the form
.
In this case we can finish integration of the given equation as follows
.
Ex. 17. Find the general solution of the second order differential equation
.
This equation doesn’t contain explicitly the unknown function.
The first step. Putting we get the first order linear equation in ,
.
By corresponding theory we put and so
,
.
The second step. Returning to we find the general solution in question,
.
3. Second order differential equation not containing explicitly the independent variable
( 27 )
reduces to the first order differential equation by introducing an auxiliary unknown function
( 28 )
Differentiating a composite function we obtain
, ( 29 )
and so
. ( 30 )
We get the first order differential equation in .
If we can find the general solution of the equation (30) in the next form
then
.
Ex. 18. Solve Cauchy problem for an equation with initial conditions .
The equation doesn’t contain explicitly the independent variable, and so we put
.
The first step.
;
by initial conditions
.
The second step.
.
On the base of the first initial condition , and the solution of Cauchy problem is given by the equality
.
Ex. 19. Solve Cauchy problem .
The first step. .
By virtue of initial conditions (verify!) and so (after division by )
.
This last differential equation is Bernoulli one, and we find its solution of the form
,
whence
.
;
; from the initial conditions
,
.
The second step.
;
The required solution of Cauchy problem
or .