- •10. Properties of integrated functions and double integrals
- •11. Double integral calculation.
- •12. Reduction of double integral to repeated one in a case of curvilinear area.
- •13. Change of variables in double integrals.
- •14. Mechanical applications of double integral.
- •15. Triple integral. Task about mass calculation. Definition and conditions of existence.
- •16. Properties of integrated function and triple integrals.
- •18. Calculation of triple integral in a case of arbitrary area.
- •19. Change of variables in triple integrals.
- •20. Harmonic analysis and periodic values.
- •21. Coefficient determination by Euler-Fourier method.
- •22.Orthogonal systems of functions.
- •24. First basic lemma.
- •26. Dini test of Fourier series’ convergence
- •27. Lipschitz test test of Fourier series’ convergence
- •29. The case of aperiodic function.
- •30. The case of arbitrary interval.
- •31. Expanding only by sines or cosines.
- •32. The complex form of Fourier series.
- •33. The extremal property of the partial sums of Fourier series.
- •34. Bessel inequality. Parswval-Steklov equality
12. Reduction of double integral to repeated one in a case of curvilinear area.
Let’s consider area (P) bounded by two curves y=y1(x) and y=y2(x) and by lines x=a and x=b.
Th 2.
If for function f(x,y) defined in area (P) double integral
exists and for any permanent value x in [a,b] simple define integral
exists then repeated integral
also exists and
(2.5)
Proof.
Proof is based on reduction of this case to considered one above in
Th 1. Let’s draw rectangle R=[a,b,c,d] containing area (P), where
![]()
and
define function f*(x,y) such that
Let’s
demonstrate that this function satisfies to conditions of Th.1. At
first it is integrated in area (P) because here it coincide with
integrated function f(x,y), therefore
.
On other hand f*(x,y)=0 out of (P) and because that is integrated in
remaining part of rectangle (R) and
.
Then according to property 2 function f* is integrated in all
rectangle (R) and
(2.6) . For
permanent value x in [a,b] there integral
exists because any of three integrals on right exist. Really, first
and third integrals exist being equal to zero and second integral
coincide with integral of function f(x,y)
.
Finally we have got
(2.7) . And according to Th.1 repeated integral exists too and is
equal to double one
.
Taking into account (2.6) and (2.7) we can see that this formula is
analogical to formula (2.5) .Q.e.d.
In a case when area is bounded by curves x=x1(y),
x=x2(y)
and by lines y=c, y=d we can got formula
(2.5*). Such areas are called first type area and second type area
accordingly. Besides that some area may be considered both as first
and second type (example). And, finally, any complex closed area may
be divided into parts representing itself areas of first or second
type.
13. Change of variables in double integrals.
Let’s
consider double integral
(1.1) where area (D) bounded by continuous curve (L) and function f
is continuous in this area. Suppose now that area (D) is connected
with another area (
)
by formulas
(1.2)
so that between points belonged to (D) and (
)
one-one mapping exists. It’s necessary to present integral (1.1)
spread in area (
)
by changing variables in it. Let’s divide area (
)
into parts (
)
(i=1,2,…,n); at the same time area (D) also will be divided into
parts (Di).
In each part (Di)
let’s choose arbitrary point (xi,yi);
and finally let’s compose the integral sum for integral (1.1)
.It’s
known that squares Di
and Δi
connected
with formula
where J is jacobian -
and
is
some point belonged area (
).
This point is defined by mean value theorem and we can’t choose it
arbitrarily, but point (xi,yi)
in area (Di)
we can take arbitrarily. Using this fact we suppose that
.
Then integral sum takes form
.
In this form it represent integral sum for integral
(1.3)
. Existence of the last integral follows from continuity of function
f. Finally, we can write
(1.4).
So, rule for changing variables in double integral: it’s necessary to change variables x and y by formulas (1.2) in integrating function and multiply integrand by jacobian.
The most
usable is polar coordinates system:
.
Jacobian for this system is
.
Then formula
(1.4) takes form
(1.5)
