- •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
3. Homogeneous de-1
Def. 11. The first order differential equation is called homogeneous one (with respect to the variables x, y) if it can be represented in the next form
. ( 15 )
Theorem 4. Homogeneous differential equation (15) as a rule reduces to that separable by introducing a new unknown function
. ( 16 )
■Finding and substituting its value in the equation we have
.
The obtained equation is a separable one provided . Indeed, in this case
.■
Note 6. It can be proved that differential equation
, ( 17 )
is that homogeneous if for any
.
A more general differential equation
( 18 )
is homogeneous one if for any there exists a number k such that simultaneously
and .
Prove these assertions yourselves.
Ex. 9. Solve Cauchy problem .
Let’s divide both sides of the equation by x. We’ll get an equation of the form (15) that is a homogeneous equation,
,
because of its right side is a function of the ratio . Acting by the theory we have
.
The initial condition gives
.
The solution of Cauchy problem
or .
Ex. 10. Find the general solution of a differential equation
.
The given equation is that homogeneous because of for any
.
To prove homogeneity of the equation directly we rewrite it in the next form
and then divide the numerator and denominator by
.
The right side of the equation is a function of the ratio , and so the equation is homogeneous one. By the theory we have
Ex. 11. Find a curve through a point if the subtangent at its arbitrary point equals the sum of coordinates of this point.
It follows from the conditions of the problem that an unknown curve can’t intersect the Ox-axis and so lies above of this axis.
Let is an equa-tion of a curve in question, and be the segments of the tangent and normal to the curve at its arbitrary point respectively, and (see fig. 2) . Then directed segments and are called respectively the subtangent and Fig. 2 subnormal to the curve at the point .
For the case (see fig. 2, where the point A lies from the left of the point N)
.
We can prove this from the right triangle , namely
;
the same value of we’ll get proceeding from the equation of the tangent to the unknown curve at the point . Indeed, the equation of the tangent is
If we put here, we’ll obtain
.
The length of the subtangent equals
,
and by the conditions of the problem we get the differential equation
with an initial condition
that is we have to solve Cauchy problem.
The first case
.
To determine the type of the equation we write it as follows
and divide the numerator and denominator of the fraction by x,
.
We get a differential equation of the form (15), and therefore it’s homogeneous one. Integrating it by corresponding method we have
.
The value of C we find by virtue of the initial condition. Substituting 0 for x and 1 for y in the general solution we get
.
The curve in question has the next equation: or .
The second case
.
Integration of the differential equation (which is also homogeneous one) gives
The initial condition is fulfiled only for : , and therefore the curve in question is given by the equation .
Answer. There are two solutions of the problem: , .