- •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 4. Nonhomogeneous equations Structure of the general solution of so lnde
Theorem 6 (structure of the general solution of the second order linear nonhomogeneous differential equation (1)). The general solution of SO LNDE equals the sum of the general solution of corresponding [associated] LHDE (3) and some particular solution of the given equation,
. ( 18 )
■ Let is the general solution of LHDE (3), where are two linearly independent solutions of LHDE. A function
is a solution of the equation (1) for any values of because of
.
We have only to prove that for any initial conditions (2) one can find values of to satisfy these conditions. Since
,
we get a system of linear equations in
which has unique solution because of its principal determinant is and doesn’t equal zero on account of linear independence of .■
Ex. 11. A function is the general solution of a differential equation .
Indeed, is the general solution of the corresponding homogeneous equation (see Ex. 6, 9), and a function is a particular solution of the given equation.
Method of variation of arbitrary constants
Let we must find the general solution of SO LNDE (1). We can do it with Lagrange in the next two steps.
1. We find the general solution
of the corresponding LHDE (3), where are its linearly independent solutions.
2. Now we find the general solution of SO LNDE (1) in the same form as , but we treat as unknown functions, namely
. ( 19 )
We find the first derivative of y,
,
and we suppose that
.
Then
.
Substituting the values of in the equation (1), we have
.
We get the next system of linear equations in
( 20 )
Solving the system (20) we get
,
where be some functions. Integrating, we have finally
( 21 )
where are arbitrary constants. The general solution of the equation (1) is
. ( 22 )
Note 1. We can represent the general solution (22) in the next form:
,
and we see that
is the general solution of the homogeneous equation (3) and
is the particular solution of the nonhomogeneous equation (1).
Ex. 12. Find the general solution of an equation .
1. Corresponding LHDE is , its characteristic equation
has real equal roots , and LHDE has linearly independent particular solutions
and the general solution
2. Now we seek the general solution of the given equation in the form
By virtue of the formula (20) the system of linear equations in and its solution are
After integration
,
and the general solution of the given differential equation
.
Ex. 13. Solve Cauchy problem .
1. For corresponding [associated] homogeneous equation linearly independent particular solutions and the general solution
.
2. We seek the general solution of the given equation in the form
,
and by virtue of (20) we get the system of equations in
or
The general solution of the given differential equation is
.
3. Determination of values of with the help of the initial conditions.
The solution of Cauchy problem
.