- •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
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
POINT 3. ORDER REDUCING SECOND ORDER DIFFERENTIAL EQUATIONS
Point 1. General notions
Def. 1. Equation with respect to an unknown function is called differential one if it contains the derivative or derivatives of this function.
Def. 2. Order of a differential equation is called the highest order of derivatives of the unknown function which contains the equation.
(
1 )
is the general form of the first order differential equation in .
( 2
)
is the general form of the second order differential equation in .
Def. 3. Solution
of a differential equation is called a function
which satisfies this equation that is turns it into identity.
For example a function
is the solution of the first order differential equation (1) if
.
Def. 4. Integral curve of a differential equation is called the graph of its solution.
Every differential equation has infinitely many solutions.
Ex. 1. Set of all solutions of a differential
equation
is given by the expression
where C is
an arbitrary constant.
To choose some certain solution of a differential equation one gives additional conditions.
There are boundary and initial conditions.
Ex. 2. Find a solution of a differential equation
which satisfies the next boundary conditions
.
In our lectures we’ll study as the rule differential equations with initial conditions.
For the first order differential equation (1) we have one initial condition name-ly
.
( 3 )
For the second order differential equation (2) we have two initial conditions
.
( 4 )
Def. 5. Problem of finding solutions of a differential equation which satisfy an initial condition or initial conditions is called the initial-value problem or Cauchy problem.
For the first order differential equation (1) we have Cauchy problem (1), (3), and for the second order differential equation (2) we have Cauchy problem (2), (4).
Geometrical sense of
Cauchy problem (1), (3): find integral curves which pass through a
given point
.
Geometrical sense of Cauchy problem (2), (4): find integral curves which pass through a given point and have at this point the given slope of a tangent.
Ex. 3. Find a curve through a point
if the
slope of the tangent at its arbitrary point
equals
.
We must solve Cauchy problem for the first order differential equation
with an initial condition
.
The equation gives
,
and from the initial condition we find the value of C,
,
and therefore
.
Theory of differential equations establishes conditions for one-valued solvabi-lity of Cauchy problems.
Let’s we study the first order differential
equation which is resolved with respect to the derivative
that is
(
5 )
Theorem 1. If a
function
in the first order differential equation (5) and its partial
derivative
with respect to y
are continuous in some domain D
of the
-plane,
then for any point
Cauchy problem (5), (3) has unique
solution.
Def. 6. General
solution of the first order differential equation (5) in the domain D
of the theorem 1 is called a function
which contains an arbitrary constant C and satisfies two conditions:
a) it is a solution of the equation for any va-lue of C; b) for any
initial condition (3) one can find a value
of C such that the function
satisfies this condition.
Def. 7. If an arbitrary constant C in the general solution of a differential equation (5) takes on some particular value then the corresponding function is called a particular solution of this equation.
For example the solution of Cauchy problem is a particular one.
Let’s now we study the second order differential
equation resolved with respect to the second derivative
(
6 )
Theorem 2. If a
function
in the differential equation (6) and its partial derivatives
with respect to
are continuous in some domain D
of the
-space,
then for any point
Cauchy problem (6), (4) has unique
solution.
Def. 8. General
solution of the second order differential equation (6) in the do-main
D of the
theorem 2 is called a function
which contains two arbitrary constants
and satisfies two conditions: a) it is a solution of the equation for
any values of
;
b) for any initial conditions (4) one can find values
,
of
such that the function
satisfies these conditions.
For any particular values
,
of
we have a particular solution y =
of the equation (6), for example the solution of Cauchy problem (6),
(4).
Note 1. The general solution or a particular solution of a differential equation can be expressed implicitly. In such case they can be called respectively the general integral or a particular integral of this equation.
Note 2. Analogous definitions and theorems are introduced for nth order differential equations (if n > 2).
In the future the expression “to solve (or to integrate) a differential equation” means: a) to find its general solution or b) to solve Cauchy problem for the equation.
