- •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. 24. Double integral
POINT 1. DOUBLE INTEGRAL
POINT 2. EVALUATION OF A DOUBLE INTEGRAL IN CARTESIAN COORDINATES
POINT 3. IMPROPER DOUBLE INTEGRAL. POISSON’S FORMULA
Point 1. Double integral
Def. 1. Let a function of two variables be given in a some domain D of the -plane (fig. 1).
1. We divide the domain into n parts with areas and diameters .
2. We take arbitrary point in every part , find the value of the function at this point and multiply it by the area of .
3. We add all these products Fig. 1 and get an integral sum
.
4. Let and . If there exists the limit of the integral sum , then this limit is called the double integral of the function over the domain D and is denoted by
( 1 )
We can consider the double integral as the sum of elements where dS = dxdy is an element of the area.
Theorem 1 (existence of a double integral). If a function is continuous in a domain D then its double integral over D exists.
It is evident that for a double integral gives the area of the domain D,
. ( 2 )
Mechanic sense of a double integral. If is the surface density of a plate , then its mass equals the next double integral
( 3 )
■An element of the mass
;
it is the mass of the element with the area and with a constant surface density (fig. 2). Sum of all these elements gives the mass of the plate which is re- Fig. 2 presented by a double integral (3).■
Def. 2. A cylindrical body [a curvilinear cylinder] is called a body bounded:
a) above by a surface ;
b) below by a domain D of the xOy-plane;
c) aside by a cylindrical surface with the generatrix parallel to -axis and the diréctrix which is the boundary of the domain Fig. 3 Fig. 4 D (fig. 3).
Geometric sense of a double integral. The volume of a cylindrical body equals the double integral
. ( 4 )
■An element of the volume
is the volume of a right circular cylinder with the base of the area and the height (fig. 4). The volume of a cylindrical body is the sum of all these elements and is represented by the double integral (4).■
Properties of a double integral are the same as for a definite integral.
For example:
1 (linearity). For any functions and any constants
.
2 (additivity). If a domain is divided into two disjoint parts , (fig. 5), then
. Fig. 5
Point 2. Evaluation of a double integral in cartesian coordinates
Def. 3. A domain D is called a domain of the first type if it is bounded (see fig. 6):
a) from the left by a straight line ;
b) from the right by a straight line ;
c) below by a line ;
d) above by a line , Fig. 6 .
A double integral over a domain of the first type is calculated by a formula
. ( 5 )
Correspondingly to this formula we integrate at first with respect to y from to , that is calculate an inner integral
, Fig. 7 and then we integrate the result with respect to x from a to b.
■We’ll prove the formula (5) proceeding from the mechanic sense of a double integral. Let the integrand be the surface density of a plate, defi-ned by the figure (fig. 6). Hence the mass of the plate equals the double integral
.
Now we’ll find the same mass by the other way and compare the results. The mass of the element of the plate between and (fig. 7) equals . Adding all such the masses from to we find the mass of the hatched strip (fig. 7), namely
.
Adding finally the masses of all such the strips from to we find the mass of the whole plate that is
.
Comparing of two results of the mass calculating proves validity of the formula (5).■
Note 1. Integral with respect to x from a to b is called that exterior [external]. The right side of the formula (5) is called the repeated integral.
Def. 4. A domain D is called a domain of the se-cond type if it is bounded (see fig. 8):
a) below by a straight line ; b) above by a a straight line ; c) from the left by a line ; d) from the right by a line , .
Fig. 8 The double integral over a domain D of the se-cond type is calculated by a formula
. ( 6 )
At first we calculate an inner integral
,
that is integrate with respect to x from to , and then we integrate the result with respect to y from c to d.
■Prove this formula yourselves.■
Ex. 1. Let a domain of integration is a rectangle
with the sides parallel to Ox-, Oy-axes (fig. 9). The rec-tangle is the domain of the first and second types, there- Fig. 9 fore we can use both formulas (5) and (6),
. ( 7 )
The formula (6) means that in the case of the rectangle we can integrate in any order. But one of orders of integration can lead to easier calculations than the other one.
Ex. 2. Find the mass of a plate
(fig. 10)
if the surface density of the plate equals . We find the mass by the formula (3). A domain of integration R is a rectangle with the sides parallel to Ox-, Oy-axes. Using the formula (7) we get Fig. 10
.
The other order of integration isn’t well (verify!).
Ex. 3. Evaluate by two ways the integral if the domain D is defined by inequalities (fig. 11).
The domain D is that of the first and second types.
The first way. We consider D as a domain of the first type,
, Fig. 11 that is D is bounded
a) from the left by the straight line ;
b) from the right by the straight line ;
c) below by the line ;
d) above by the line .
Using the formula (5) we have
In the second way we treat D as a domain of the second type,
,
that is D is bounded
a) below by the straight line ;
b) above by the straight line ;
c) from the left by the line ;
d) from the right by the line .
Therefore with the help of the formula (6) we write
.
Fulfill evaluation of the integral yourselves.
Ex. 4. Set the limits of integration in a double integral over a triangular domain D with the vertices
Fig. 12 (fig. 12)
At first we compile the equations of the straight lines OA and AB.
OA:
AB: .
The first way. The domain D is that of the first type because of it’s bounded from the left by a straight line x = 0, from the right by a straight line x = 5, below by a line , above by a line hence on the base of the formula (5)
.
The second way. To apply the formula (6) we divide the domain D into two domains of the second type by a straight line y = 4 (fig. 12). If we describe them by two double inequalities, namely
we’ll get
Ex. 5. Evaluate the double integral
Fig. 13 over the domain
(fig. 13).
The domain D is that of the first type. It can be divided into two domains of the se-cond type by the straight line
(fig. 13),
,
,
.
The integral in question equals the sum of two integrals. It’s well to calculate
the first one over the domain D and the second one as the sum of integrals over and .
.