2. Laxmi Institute of Technology ,
Sarigam
Branch: Mechanical Engineering
Div.: A
Subject : CALCULUS
Guided By : Mr. GAURAV GANDHI , Mr. DARPAN BULSARA
Prepared By : Roll no. 23 - 33
4. contents:
Double integral
Fubini’s theorem
Algebraic Properties
Double integrals in polar
coordinate
Triple integration
5. MULTIPLE INTEGRALS
DOUBLE INTEGRALS
Let the function z=f(x,y) be defined on some region R
Divide the region R into small parts by drawing lines parallel to X-axis and Y-axis within the region
R.
These parts are in the form of rectangle of lengths x &
,except some of the parts at the boundaries of the region.
Let the number of such rectangles be n. Each of area
Choose any point in any area
If we take then all the small parts wthin the region will approximately behave like
rectangles.
k k x y
Then the following limit of sums over region R :
y
( *, *) A x* y
n
lim ( *, *)
1
n
n k k k
k
f x y A
6. {( , , ) 0 ( , ),( , ) } 3 s x y z R z f x y x y R
7. MULTIPLE INTEGRAL
DOUBLE INTEGRAL
Is known as the double integral of f(x,y) over R and can be written as
f (x, y)dA
8. MULTIPLE INTEGRAL
Fubini’s theorm
If f(x,y) is continuous throught the rectangular region
f ( x , y ) dA f ( x , y )
dxdy
f x y dA f x y dydx
&
d b
R c a
b d
( , ) ( , )
R a c
d b d b
f ( x , y ) dxdy [ f ( x , y ) dx ]
dy
c a c a
9. MULTIPLE INTEGRAL
For example
2 1
(13xy)dxdy
1 0
2 2
x y
1
0
I x dy
1
3
[ ]
2
2
I dy
1
3
y
(1 )
2
2
2
1
3
y
y
[ ]
4
12 3
[2 1 ]
4 4
3
4
4
10. MULTIPLE INTEGRAL
Algebraic properties
Properties:
1. cf(x,y)dA
c f(x,y)dA
R R
2. (f(x,y) g(x,y))dA f(x,y)dA
g(x,y)dA
R R R
3. If f(x,y) g(x,y) (x,y)
R, then
R R
R
f(x,y)dA g(x,y)dA
4 f(x,y) dA 0, if f (x, y) 0 on R
11. CHANGE TO POLAR COORDINATES
Suppose that we want to evaluate a double
integral , where R is one of the regions
shown here
12. CHANGE TO POLAR COORDINATES
Double integrals in polar coordinate
From this figure the polar coordinates (r, θ) of a point are
related
to the rectangular coordinates (x, y) by
the equations
r2 = x2 + y2
x = r cos θ
y = r sin θ
The regions in the first figure are special cases of a polar
rectangle
R = {(r, θ) | a ≤ r ≤ b, α ≤ θ ≤ β}
shown here.
13. CHANGE TO POLAR COORDINATES
To compute the double integral
where R is a polar rectangle, we divide:
The interval [a, b] into m subintervals [ri–1, ri]
of equal width Δr = (b – a)/m.
The interval [α ,β] into n subintervals [θj–1, θi]
of equal width Δθ = (β – α)/n.
14. CHANGE TO POLAR COORDINATES
Then, the circles r = ri and the rays θ = θi
divide the polar rectangle R into the small
polar rectangles shown here
15. CHANGE TO POLAR COORDINATES
The “center” of the polar subrectangle
Rij = {(r, θ) | ri–1 ≤ r ≤ ri, θj–1 ≤ θ ≤ θi}
has polar coordinates
ri* = ½ (ri–1 + ri)
θj* = ½(θj–1 + θj)
16. CHANGE TO POLAR COORDINATES
The rectangular coordinates of the center
of Rij are (ri* cos θj*, ri* sin θj*).
18. Triple integrals
We consider a continuous function f(x,y,z) defined over a
bounded by a solid region D in three dimensional space .We
divide a solid region D into small rectangular parallelepiped
by drawing planes parallel to coordinate planes .
Consider any point in one of the cells with
volume
If we partition the solid region D into large number of such cells
then the following limits of the approximation of sum
Vk xk . yk . zk
19. Triple integrals
Is known as triple integral of f(x,y,z) over D and can be written as:
Example 1
Evaluate the triple integral
where B is the rectangular box
21. DEFINITION The Jacobian of the transformation T
given by x= g (u, v) and
y= h (u, v) is
y
u
x
v
y
v
x
u
x
y
v
x
y
u
v
u
x y
( , )
( , )
u v
22. CHANGE OF VARIABLES IN A DOUBLE INTEGRAL Suppose
that T is a C1
transformation whose Jacobian is nonzero and that maps
a region S in the uv-plane onto a region R in the xy-plane.
Suppose that f is continuous on R and that R and S are type
I or type II plane regions. Suppose also that T is one-to-one,
except perhaps on the boundary of . S. Then
( , )
R S
dudv
x y
u v
f x y dA f x u v y u v
( , )
( , ) ( ( , ), ( , ))
23. Let T be a transformation that maps a region S in
uvw-space onto a region R in xyz-space by means of
the equations
x=g (u, v, w) y=h (u, v, w) z=k (u, v, w)
The Jacobian of T is the following 3X3 determinant:
24.
R
x y z
( , , )
( u , v , w
)
f (x, y, z)dV
x
w
y
w
z
w
x
v
y
v
z
v
x
u
y
u
z
u
s
dudvdw
x y z
( , , )
u v w
f x u v w y u v w z u v w
( , , )
( ( , , ), ( , , ), ( , , ))