
- •Міністерство освіти і науки україни донецький національний технічний університет
- •Integral calculus (інтеґральне числення)
- •Донецьк 2005
- •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 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 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
- •Simpson’s 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
- •Contents
- •Integral calculus 3
- •Integral calculus (Інтеґральне числення): Методичний посібник по вивченню розділу курсу ”Математичний аналіз” для студентів ДонНту (англійською мовою)
Lecture no. 21. Definite integral
POINT 1. PROBLEMS LEADING TO THE NOTION OF A DEFINITE INTEGRAL
POINT 2. DEFINITE INTEGRAL
POINT 3. PROPERTIES OF A DEFINITE INTEGRAL
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
Point 1. Problems leading to the concept ofa definite integral
P
roblem
1. Area of a curvilinear trapezium
Def. 1. Curvilinear
trapezium on the
-plane
is called a figure bounded by two straight lines
,
,
-axis
and a curve
(fig.1). It’s useful to denote a curvilinear trapezium as
Fig. 1 the next set of points of the -plane
.
( 1 )
To define the notion of the area of the curvilinear trapezium (1), fig.1, we car-ry out the next construction.
1. With the help of points
we divide the segment into n parts (subintervals)
of the lengths
,
and
let
.
2. We take arbitrary point
in every part
find the value of the function at this point and multiply it by
.
3. Adding all these products
we
get a sum
( 2 )
-
area of a step-type figure generated by rectangles with bases
and altitudes
.
4. Let tends to zero. If there exists the limit of the sum (2), it is called the area of the curvilinear trapezium (1) (fig.1) and is denoted
.
( 3 )
Problem 2. Produced quantity
Let
is a labour productivity of some factory at a time moment t.
Find its produced quantity
during a time interval
.
If
,
then
.
But as a rule
,
and we must do as follows.
1. We divide the time segment 0, T into n parts
,
and let
.
2. We take arbitrary point
in every part
find the value of the function
at this point and multiply it by
.
3. Adding all the products
we find an approximate value of the
produced quantity
during 0,
T,
that is
.
( 4 )
4. Tending
to zero we find the exact value of the produced quantity
.
( 5 )
Problem 3. Length path.
Find the length path L
traveled by a material point with a given velocity
during a time interval T
(from the moment of time t
= 0).
If
then
.
For a variable velocity we do by the same way as in preceding problems.
1. We divide the interval 0, T into n parts
and put
.
2. In every time interval we take arbitrary moment , find the value of the velocity at this moment and multiply it by .
3. Adding all the products
we find approximate value of the
length path L
traveled by a material point during 0,
T,
that is
.
( 6 )
4. Tending to zero we find the exact value of the length path L
.
( 7 )