- •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
Lecture no.26. Second order linear differential equations
POINT 1. GENERAL NOTIONS
POINT 2. LINEAR DEPENDENCE AND INDEPENDENCE
POINT 3. HOMOGENEOUS EQUATIONS
POINT 4. NONHOMOGENEOUS EQUATIONS
Point 1. General notions
Def. 1. The second order linear differential equation (SO LDE, LDE) is called the next equation
.
( 1 )
Coefficients
and the second [free, absolute] term
of equation are known functions,
is an unknown function.
Initial conditions for the equation (1) have a usual form
( 2 )
Equation (1) is called nonhomogeneous one (SO LNDE, LNDE) if its second term doesn’t equal zero identically.
If
,
the corresponding [associated] equation
( 3 )
is called homogeneous equation (SO LHDE, LHDE) which corresponds to the (non-homogeneous) equation (1).
Theorem 1 (on
one-valued solvability of Cauchy problem).
If coefficients
and a second term
of the equation (1) are continuous functions on some segment
then Cauchy problem (1), (2) (in particular (3), (2)) has unique
solution, and this solution is determined on the whole segment
.
Ex. 1. Cauchy’s problem for homogeneous equation (3) with zero initial conditions
( 4 )
has
unique trivial solution
.
Def. 2. The left
side of the differential equations (1), (3) is called a linear
differential operator and is denoted by
,
.
( 5 )
The linear differential operator possesses evident properties
1.
(additivity).
■
.■
2.
for any constant k (homogeneity).
■
■
As the corollary we have
for
any constant
(linearity).
With the help of the linear differential operator the equations (1), (3) can be written as follows
,
.
Properties of solutions of a linear homogeneous differential equation (3).
1. Sum of two solutions of the equation (3) is also a solution.
■Let
be solutions of the equation (3) that is
.
By the property 1 of a linear differential operator
.■
2. Product of any solution of the equation (3) by a constant is also a solution.
■Let y is
a solution of the equation (3), i.e.
,
and k is a
constant. Then by the property 2 of a linear differential operator
.■
3. If a function
is
a complex solution of the equation (3) then its real and imaginary
parts
are
also the solutions of this equation.
Point 2. Linear dependence and independence
Def. 3. Two
functions
are called linearly dependent
on a segment
if there exist two numbers
not all zeros (
)
such that for any
an identity
( 6 )
holds.
If the identity holds only in the case
,
these functions are called li-nearly
independent.
Theorem 2. Two
functions
are linearly dependent on a segment
if and only if their ratio identically equals a constant on
,
that is for any
.
( 7 )
■1. Let functions
are linearly dependent on a segment
,
and so the identity (5) holds for
.
If, for example,
then we get from (6)
and a ratio of functions is an identical constant.
2. Let now
on
.
Then
,
and are linearly dependent by the definition of linear dependence.■
Ex. 2. Functions
for
are
linearly independent on
because of their ratio isn’t a constant.
Def. 4. n
functions
are called linearly dependent on a segment
if there exist n
numbers
not all zeros (
)
such that for any
an identity
( 8 )
holds.
If the identity holds only in the case
,
these functions are called linearly
independent on
.
Ex. 3. Functions
are
linearly independent on
because of a polynomial in x
only
if all its coefficients equal zero, i.e.
.
In what follows we’ll deal with linear dependence or independence of solutions of differential equations. There is well mathematical tool to study corresponding questions namely the wronskian [Wronskian determinant, determinant of Wronski] of several functions.
Def. 5. Wronskian
of functions
is called the next determinant
( 9 )
Ex. 4. The wronskian of functions (see Ex. 2) is
.
Theorem 3. If
functions
are linearly dependent on a segment
then their wronskian identically equals zero on
,
.
■Let for the sake of simplicity two functions are linearly dependent on .
The first mode
of proving. The ratio of the functions
is identical constant on
.
Let for example
.
Then the wronskian of these functions
.
The second mode
of proving (it can be easily extended on any number of functions). By
the definition of linear dependence there are two numbers
such that
and
on
.
We differentiate this identity and compile a system of linear
homogeneous equations in
,
This system has non-trivial solution, and therefore its principal determinant equals zero for any ,
.■
Theorem 4. If functions are linearly independent solutions of the nth order linear homogeneous differential equation with coefficients continuous on a segment , then the wronskian of these solutions doesn’t equal zero at all the points of the segment.
■Let’s prove the theorem for two linearly
independent solutions
of the second order linear homogeneous differential equation (3).
Suppose that the wronskian of these functions equals zero at a point
,
.
We choose two numbers
such that
and
( 10 )
It’s
possible because the system (10) in
has zero principal determinant
.
Let’s compile the next function
.
It is a solution of the equation (3) and satisfies zero initial conditions (10). Hence on the base of Ex. 1 y = 0, that is
.
But it means that the functions are linearly dependent (we remember that ).
We’ve arrived at contradiction which proves the theorem.■
Ex. 5. The functions
(see Ex. 2) are linearly independent solutions of a differential
equation
on
.
Their wronskian equals
(see Ex. 4) and doesn’t equal zero for any
.
