SlideShare a Scribd company logo
Triple Integral
Definition of the Triple Integral
Theorem for Evaluating Triple Integrals
Theory
 Meaning
Rules For Solving
Polar ( cylindrical ) Coordinates
Examples
References
Let f(x,y,z) be a continuous function of three variables defined over a solid Q. Then
the triple integral over Q is defined as
∭ 𝑓( 𝑥, 𝑦, 𝑧) = 𝑙𝑖𝑚 ∑ 𝑓( 𝑥, 𝑦, 𝑧)∆𝑥∆𝑦∆𝑧
𝑄
where the sum is taken over the rectangular solids included in the solid Q and lim is
taken to mean the limit as the side lengths of the rectangular solid.
DefinitionoftheTripleIntegral
Let f(x,y,z) be a continuous function over a solid Q defined by
a < x < b h1(x) < y < h2(x) g1(x,y) < z < g2(x,y)
Then the triple integral is equal to the triple iterated integral.
TheoremforEvaluatingTripleIntegrals
∭ f(x, y, z) = ∫ ∫ ∫ f(x, y,z, )dz dy dx
g2(x,y)
g1(x,y)
h2(x)
h1(x)
b
a𝑄
 As the name implies, triple integrals are 3 successive integrations, used
to calculate a volume, or to integrate in a 4th dimension, over 3 other
independent dimensions. Examples:
Theory
∭ 𝑓 ( 𝑥, 𝑦, 𝑧) 𝑑𝑉
𝑉
0
∫ ∫ 1
3X−2
0
5
1
∫ (2X + eyz)dz dy dx
COS(X+Y)
SIN(X+Y)
∫ 1
2𝜋
0
∫ 1
2
0
∫ 𝑟 𝑑𝑧 𝑑𝑟 𝑑𝜃
3
−3
 To understand triple integrals, it is extremely important to have an
understanding of double integrals, coordinate geometry in 3 dimensions,
and polar (cylindrical) coordinates. Sums of triple integrals are based on
these topics and cannot be solved without this prior knowledge.
 Just as a single integral over a curve represents an area (2D), and a double
integral over a curve represents a volume (3D), a triple integral represents a
summation in a hypothetical 4th dimension. To understand this, imagine a
slightly different scenario, where the first 3 dimensions are space, space, and
time, and that the fourth dimension is the third space dimension: suppose
you have an integral of z where z is a function of x, y, and t, and x and y are
also functions of t. Integrating z with respect to x and y gives us the volume
as a function of t. If we plug in a value for t, this gives us the numerical
volume at a particular instance of time.
Meaning
 However, as the volume is a function of t, it changes with respect to time.
Thus, if we integrate this result with respect to t, we are adding up all the
different volumes over a period of time. For example, imagine a balloon that
is being inflated. At any particular instant of time, we can use a double
integral to calculate its volume. However, if we wanted to sum up all the
volumes over the entire inflation process, we must use a triple integral as
described above.
Meaning(Contd.)
 Triple Integrals can also be used to represent a volume, in the same way that
a double integral can be used to represent an area. In the triple integral
∫ ∫ ∫ 𝑓 ( 𝑥, 𝑦, 𝑧 ) 𝑑𝑧 𝑑𝑦 𝑑𝑥
𝑧
0
𝑏
𝑎
𝑑
𝑐
If 𝑓( 𝑥, 𝑦, 𝑧, ) = 1 then this triple integral is the same as
∫ ∫ 𝑧 ( 𝑥, 𝑦 ) 𝑑𝑦 𝑑𝑥
𝑏
𝑎
𝑑
𝑐
Which is simply the volume under the surface represented by 𝑧 ( 𝑥, 𝑦 ) .
RulesForSolving
 In general, if you are evaluating a triple integral of f( x,y,z ) over a volume V, by
properly choosing the limits, you can integrate with respect to the 3 variables
in any order. For example, if V represents a rectangular box, then for x, y, and
z, the limits of integration will all be constants and the order does not matter
at all.
∫ ∫ ∫ 𝑓 𝑑𝑧 𝑑𝑦 𝑑𝑥 = ∫ ∫ ∫ 𝑓 𝑑𝑥 𝑑𝑧 𝑑𝑦 = ⋯
𝑓
𝑒
𝑏
𝑎
𝑑
𝑐
𝑏
𝑎
𝑑
𝑐
𝑓
𝑒
and so on, for 6 different possible orders of integration.
Now consider the case where you want to find the triple integral
∭ 𝑓 ( 𝑥, 𝑦, 𝑧 ) 𝑑𝑉
𝑉
0
where V is the volume under the plane
𝑧+2𝑥+3𝑦=6, in the first quadrant.
Since V is in the first quadrant, it is bounded by the 3 planes 𝑥=0,𝑦=0,𝑧=0 in
addition to the plane whose equation is given above.
Clearly, the shape of V is a tetrahedron with the vertices (3,0,0), (0,2,0), (0,0,6),
and (0,0,0).
One way to set up the integral is to first consider the z direction. In this direction
we enter through 𝑧=0 and leave through 𝑧=6−2𝑥−3𝑦. If we do this first, then
we can consider the x or y direction next. If y, we enter through 𝑦=0, and leave
through 𝑦 = −
2
3
𝑥 + 2. Thus, x must be given the limits 0 to 3, and our triple
integral is:
∫ ∫ ∫ 𝑓 ( 𝑥, 𝑦, 𝑧) 𝑑𝑧 𝑑𝑦 𝑑𝑥
6−2𝑥−3𝑦
0
−
2
3
𝑥+2
0
3
0
Consider the same volume, but now first we will go through in the x direction. In
this direction we enter through x=0 and leave through 𝑥=
1
2
(6−𝑧−3𝑦). If we do
this first, then we can consider the z or y direction next. If y, we enter through
𝑦=0, and leave through 𝑦=−
1
3
𝑧+2, and z must be from 0 to 6. Thus the integral
would be
∫ ∫ ∫ 𝑓 ( 𝑥, 𝑦, 𝑧 ) 𝑑𝑥 𝑑𝑦 𝑑𝑧
1
2
(6−𝑧−3𝑦)
0
−
1
3
𝑧+2
0
6
0
Both these integrals are correct and either one can be used to solve the sum and
obtain the same value. It is important to see that choosing the order of
integration depends on how the limits are chosen. However, this is entirely
independent of the function 𝑓(𝑥,𝑦,𝑧). In the first case, z must be integrated first,
since the limits were chosen such that z is dependent on (x,y). After this, since y
is chosen to be dependent on x, y is integrated next. Lastly, x as the most
independent variable is integrated. It is important to note that the third
(outermost) integral MUST always have limits of integration that are constants,
and the result should be a number. If any variables are surviving after the
integral is evaluated, most probably you have made a mistake somewhere.
Polar(cylindrical)Coordinates
Triple integrals can also be used with polar coordinates in the exact same
way to calculate a volume, or to integrate over a volume. For example:
∫ ∫ ∫ 𝑟 𝑑𝑧 𝑑𝑟 𝑑𝜃
3
−3
2
0
2𝜋
0
is the triple integral used to calculate the volume of a cylinder of height 6 and
radius 2. With polar coordinates, usually the easiest order of integration is 𝑧, then
𝑟 then 𝜃 as shown above, though it is not necessary to do it in this order.
NOTE: It is very important to remember that in polar and cylindrical
coordinates, there is an extra 𝒓 in the integral, just like in double integrals. It is
very easy to forget this 𝒓 which will lead to a wrong answer.
1. Integrate the function 𝑓(𝑥,𝑦,𝑧)=𝑥𝑦 over the volume enclose by the planes
𝑧=𝑥+𝑦 and 𝑧=0, and between the surfaces 𝑦=𝑥2 and 𝑥=𝑦2.
SOLUTION:
Since z is expressed as a function of (x,y), we should integrate in the z direction first.
After this we consider the xy-plane. The two curves meet at (0,0) and (1,1). We can
integrate in x or y first. If we choose y, we can see that the region begins at 𝑦=𝑥2
and ends at 𝑦=√𝑥, and so x is between 0 and 1. Thus the integral is:
∫ ∫ ∫ f(x, y, z)dz dy dx
x+y
0
√x2
x2
1
0
∫ ∫ 𝑥𝑦 (
𝑧 = 𝑥 + 𝑦
𝑧 = 0
[ 𝑧]) 𝑑𝑦𝑑𝑥
√ 𝑥
𝑥2
1
0
∫ ∫ xy(x + y)dy dx
√x
x2
1
0
∫ ∫ ( 𝑥2
𝑦 + 𝑦2
𝑥) 𝑑𝑦 𝑑𝑥
√ 𝑥
𝑥2
1
0
∫
𝑦 = √ 𝑥
𝑦 = 𝑥2
(
𝑥2
𝑦2
2
+
𝑦3
𝑥
3
) 𝑑𝑥
1
0
1
2
∫ ( 𝑥2
√ 𝑥
2
− 𝑥2( 𝑥2) 2) 𝑑𝑥 +
1
3
∫ (√ 𝑥
3
𝑥 − ( 𝑥2)3
𝑥)𝑑𝑥
1
0
1
0
1
2
∫ ( 𝑥3
− 𝑥6) 𝑑𝑥 +
1
3
∫ ( 𝑥
5
2 − 𝑥7) 𝑑𝑥
1
0
1
0
1
2
(
1
4
−
1
7
) +
1
3
(
2
7
−
1
8
) =
3
28
Examples
2. In the following integral, exchange the order of integrationof y and z:
∫ ∫ ∫ f(x, y,z)dz dy dx
1−y
0
1
√x
1
0
SOLUTION:
With a problem like this, it helps to draw the figure enclose by the surfaces. From
the integrals, it can be seen that z enters the volume at 𝑧=0 and leaves through
the plane 𝑧=1−𝑦. In the 𝑥𝑦 plane, 𝑦 enters through 𝑦=√ 𝑥 and leaves through
𝑦=1. These 2 conditions alone are enough to draw the figure and see that
0≤𝑥≤1.
The shape is like a tetrahedron with the vertices A(0,0,0), B(0,0,1), C(1,1,0), and
D(0,1,0), but with a curved surface between vertices A, B, C.
Rewriting the equation of the plane as 𝑦=1−𝑧, and looking at this figure,
clearly, √ 𝑥≤𝑦≤1−𝑧. Consider the projection of this surface in the 𝑧𝑥 plane. It is
a 3-sided figure bounded by 𝑥=0,𝑧=0,and 𝑧=1−√ 𝑥.
Again, it can be seen that these conditions are sufficient to obtain the limits of x
as 0≤𝑥≤1.
Thus, the integral is:
∫ ∫ ∫ f(x, y,z)dy dz dx
1−z
√x
1−√x
0
1
0
3. Evaluate ∭ 𝐸 xdV where E is enclosed by 𝑧=0,𝑧=𝑥+𝑦+5,𝑥2+𝑦2=4 and
𝑥2+𝑦2=9.
SOLUTION:
We will use cylindrical coordinates to easily solve this sum. Converting the
given outer limits of E we get: 𝑧=0,𝑧=𝑟cosθ+𝑟sinθ+5,𝑟=2 and 𝑟=3. Since
there is no limitation on the values of θ, we assume it has the values of 0 to
2π. This is also in accordance with the diagram which is obtained by drawing
these surfaces. Also, we substitute 𝑥=𝑟cosθ in the argument of the integral.
Thus the integral is:
∫ ∫ ∫ (𝑟 cos 𝜃)𝑟 𝑑𝑧 𝑑𝑟 𝑑𝜃
𝑟𝑐𝑜𝑠 𝜃+𝑟 sin 𝜃+5
0
3
2
2𝜋
0
= ∫ ∫ (𝑟2
cos 𝜃) (𝑟 cos 𝜃 + 𝑟 sin 𝜃 + 5) 𝑑𝑟 𝑑𝜃
3
2
2𝜋
0
∫
𝑟 = 3
𝑟 = 2
[
𝑟4
4
𝑐𝑜𝑠2
𝜃 +
𝑟4
4
cos 𝜃 sin 𝜃 +
5
3
𝑟3
cos 𝜃]
2𝜋
0
𝑑𝜃
∫ [
65
8
(1 + cos 2𝜃) +
65
8
𝑠𝑖𝑛 (2𝜃) +
95
3
cos 𝜃]
2𝜋
0
𝑑𝜃
=
65
8
(2𝜋 + 0 −
1
2
+ 0 − 0 +
1
2
) +
95
3
(0)
=
65𝜋
4
References
 Calculus – Sixth Edition James Stewart
 Rohit Agarwal – Math Scholar at Academic Resource Center
 Illinois Institute of Technology
 WIKIPEDIA

More Related Content

What's hot

vector space and subspace
vector space and subspacevector space and subspace
vector space and subspace
2461998
 
Partial Differentiation & Application
Partial Differentiation & Application Partial Differentiation & Application
Partial Differentiation & Application
Yana Qlah
 
Divrgence theorem with example
Divrgence theorem with exampleDivrgence theorem with example
Divrgence theorem with example
Dhwanil Champaneria
 
Taylor series and maclaurin with exercices
Taylor series and maclaurin with exercicesTaylor series and maclaurin with exercices
Taylor series and maclaurin with exercicesHernanFula
 
Methods of solving ODE
Methods of solving ODEMethods of solving ODE
Methods of solving ODE
kishor pokar
 
Green Theorem
Green TheoremGreen Theorem
Green Theorem
Sarwan Ursani
 
Series solution to ordinary differential equations
Series solution to ordinary differential equations Series solution to ordinary differential equations
Series solution to ordinary differential equations
University of Windsor
 
rank of matrix
rank of matrixrank of matrix
rank of matrix
Siddhi Agrawal
 
Power series convergence ,taylor & laurent's theorem
Power series  convergence ,taylor & laurent's theoremPower series  convergence ,taylor & laurent's theorem
Power series convergence ,taylor & laurent's theorem
PARIKH HARSHIL
 
Coordinate system
Coordinate systemCoordinate system
Coordinate system
MOHAMMAD AKRAM
 
Vector Space.pptx
Vector Space.pptxVector Space.pptx
Vector Space.pptx
Dr Ashok Tiwari
 
Orthogonal Vector Spaces
Orthogonal Vector Spaces Orthogonal Vector Spaces
Orthogonal Vector Spaces
Sohaib H. Khan
 
Gram-Schmidt process
Gram-Schmidt processGram-Schmidt process
Gram-Schmidt process
Burhanuddin Kapadia
 
Lesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General RegionsLesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General RegionsMatthew Leingang
 
B.tech ii unit-4 material vector differentiation
B.tech ii unit-4 material vector differentiationB.tech ii unit-4 material vector differentiation
B.tech ii unit-4 material vector differentiation
Rai University
 
Numerical Differentiation and Integration
 Numerical Differentiation and Integration Numerical Differentiation and Integration
Numerical Differentiation and Integration
Meenakshisundaram N
 
14.6 triple integrals in cylindrical and spherical coordinates
14.6 triple integrals in cylindrical and spherical coordinates14.6 triple integrals in cylindrical and spherical coordinates
14.6 triple integrals in cylindrical and spherical coordinates
Emiey Shaari
 
Numerical differentiation
Numerical differentiationNumerical differentiation
Numerical differentiationandrushow
 
the fourier series
the fourier seriesthe fourier series
the fourier seriessafi al amu
 
Vector calculus
Vector calculusVector calculus
Vector calculus
Melvin Cabatuan
 

What's hot (20)

vector space and subspace
vector space and subspacevector space and subspace
vector space and subspace
 
Partial Differentiation & Application
Partial Differentiation & Application Partial Differentiation & Application
Partial Differentiation & Application
 
Divrgence theorem with example
Divrgence theorem with exampleDivrgence theorem with example
Divrgence theorem with example
 
Taylor series and maclaurin with exercices
Taylor series and maclaurin with exercicesTaylor series and maclaurin with exercices
Taylor series and maclaurin with exercices
 
Methods of solving ODE
Methods of solving ODEMethods of solving ODE
Methods of solving ODE
 
Green Theorem
Green TheoremGreen Theorem
Green Theorem
 
Series solution to ordinary differential equations
Series solution to ordinary differential equations Series solution to ordinary differential equations
Series solution to ordinary differential equations
 
rank of matrix
rank of matrixrank of matrix
rank of matrix
 
Power series convergence ,taylor & laurent's theorem
Power series  convergence ,taylor & laurent's theoremPower series  convergence ,taylor & laurent's theorem
Power series convergence ,taylor & laurent's theorem
 
Coordinate system
Coordinate systemCoordinate system
Coordinate system
 
Vector Space.pptx
Vector Space.pptxVector Space.pptx
Vector Space.pptx
 
Orthogonal Vector Spaces
Orthogonal Vector Spaces Orthogonal Vector Spaces
Orthogonal Vector Spaces
 
Gram-Schmidt process
Gram-Schmidt processGram-Schmidt process
Gram-Schmidt process
 
Lesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General RegionsLesson 19: Double Integrals over General Regions
Lesson 19: Double Integrals over General Regions
 
B.tech ii unit-4 material vector differentiation
B.tech ii unit-4 material vector differentiationB.tech ii unit-4 material vector differentiation
B.tech ii unit-4 material vector differentiation
 
Numerical Differentiation and Integration
 Numerical Differentiation and Integration Numerical Differentiation and Integration
Numerical Differentiation and Integration
 
14.6 triple integrals in cylindrical and spherical coordinates
14.6 triple integrals in cylindrical and spherical coordinates14.6 triple integrals in cylindrical and spherical coordinates
14.6 triple integrals in cylindrical and spherical coordinates
 
Numerical differentiation
Numerical differentiationNumerical differentiation
Numerical differentiation
 
the fourier series
the fourier seriesthe fourier series
the fourier series
 
Vector calculus
Vector calculusVector calculus
Vector calculus
 

Similar to Triple Integral

Triple_Integrals.pdf
Triple_Integrals.pdfTriple_Integrals.pdf
Triple_Integrals.pdf
SalimSaleh9
 
Lecture 1.2 quadratic functions
Lecture 1.2 quadratic functionsLecture 1.2 quadratic functions
Lecture 1.2 quadratic functions
narayana dash
 
Change variablethm
Change variablethmChange variablethm
Change variablethm
Jasonleav
 
Lecture 3 - Linear Regression
Lecture 3 - Linear RegressionLecture 3 - Linear Regression
Lecture 3 - Linear Regression
Harsha Vardhan Tetali
 
Lecture 1.6 further graphs and transformations of quadratic equations
Lecture 1.6 further graphs and transformations of quadratic equationsLecture 1.6 further graphs and transformations of quadratic equations
Lecture 1.6 further graphs and transformations of quadratic equations
narayana dash
 
Helmholtz equation (Motivations and Solutions)
Helmholtz equation (Motivations and Solutions)Helmholtz equation (Motivations and Solutions)
Helmholtz equation (Motivations and Solutions)
Hassaan Saleem
 
Integral dalam Bahasa Inggris
Integral dalam Bahasa InggrisIntegral dalam Bahasa Inggris
Integral dalam Bahasa Inggris
immochacha
 
3 d scaling and translation in homogeneous coordinates
3 d scaling and translation in homogeneous coordinates3 d scaling and translation in homogeneous coordinates
3 d scaling and translation in homogeneous coordinates
KRIPA SHNAKAR TIWARI
 
conference_poster_5_UCSB
conference_poster_5_UCSBconference_poster_5_UCSB
conference_poster_5_UCSBXining Li
 
MA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docx
MA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docxMA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docx
MA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docx
infantsuk
 
Developing Expert Voices
Developing Expert VoicesDeveloping Expert Voices
Developing Expert Voicessuzanne
 
math vysh.pptx
math vysh.pptxmath vysh.pptx
math vysh.pptx
Vyshali6
 
121593320 teorema-stokes
121593320 teorema-stokes121593320 teorema-stokes
121593320 teorema-stokes
saidattamimi1
 
Trapezoidal Method IN Numerical Analysis
Trapezoidal Method IN  Numerical AnalysisTrapezoidal Method IN  Numerical Analysis
Trapezoidal Method IN Numerical Analysis
Mostafijur Rahman
 
Lesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptx
Lesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptxLesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptx
Lesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptx
ErlenaMirador1
 
Lesson 6 differentials parametric-curvature
Lesson 6 differentials parametric-curvatureLesson 6 differentials parametric-curvature
Lesson 6 differentials parametric-curvature
Lawrence De Vera
 
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
IOSR Journals
 
Machine learning (10)
Machine learning (10)Machine learning (10)
Machine learning (10)NYversity
 
Applications of Differential Calculus in real life
Applications of Differential Calculus in real life Applications of Differential Calculus in real life
Applications of Differential Calculus in real life
OlooPundit
 

Similar to Triple Integral (20)

Triple_Integrals.pdf
Triple_Integrals.pdfTriple_Integrals.pdf
Triple_Integrals.pdf
 
Lecture 1.2 quadratic functions
Lecture 1.2 quadratic functionsLecture 1.2 quadratic functions
Lecture 1.2 quadratic functions
 
Change variablethm
Change variablethmChange variablethm
Change variablethm
 
Lecture 3 - Linear Regression
Lecture 3 - Linear RegressionLecture 3 - Linear Regression
Lecture 3 - Linear Regression
 
Lecture 1.6 further graphs and transformations of quadratic equations
Lecture 1.6 further graphs and transformations of quadratic equationsLecture 1.6 further graphs and transformations of quadratic equations
Lecture 1.6 further graphs and transformations of quadratic equations
 
Helmholtz equation (Motivations and Solutions)
Helmholtz equation (Motivations and Solutions)Helmholtz equation (Motivations and Solutions)
Helmholtz equation (Motivations and Solutions)
 
Integral dalam Bahasa Inggris
Integral dalam Bahasa InggrisIntegral dalam Bahasa Inggris
Integral dalam Bahasa Inggris
 
3 d scaling and translation in homogeneous coordinates
3 d scaling and translation in homogeneous coordinates3 d scaling and translation in homogeneous coordinates
3 d scaling and translation in homogeneous coordinates
 
conference_poster_5_UCSB
conference_poster_5_UCSBconference_poster_5_UCSB
conference_poster_5_UCSB
 
MA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docx
MA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docxMA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docx
MA 243 Calculus III Fall 2015 Dr. E. JacobsAssignmentsTh.docx
 
Developing Expert Voices
Developing Expert VoicesDeveloping Expert Voices
Developing Expert Voices
 
math vysh.pptx
math vysh.pptxmath vysh.pptx
math vysh.pptx
 
121593320 teorema-stokes
121593320 teorema-stokes121593320 teorema-stokes
121593320 teorema-stokes
 
Trapezoidal Method IN Numerical Analysis
Trapezoidal Method IN  Numerical AnalysisTrapezoidal Method IN  Numerical Analysis
Trapezoidal Method IN Numerical Analysis
 
Lesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptx
Lesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptxLesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptx
Lesson 2-2 - Math 8 - W2Q2_Slopes and Intercepts of Lines.pptx
 
Lesson 6 differentials parametric-curvature
Lesson 6 differentials parametric-curvatureLesson 6 differentials parametric-curvature
Lesson 6 differentials parametric-curvature
 
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
Existence Theory for Second Order Nonlinear Functional Random Differential Eq...
 
returika
returikareturika
returika
 
Machine learning (10)
Machine learning (10)Machine learning (10)
Machine learning (10)
 
Applications of Differential Calculus in real life
Applications of Differential Calculus in real life Applications of Differential Calculus in real life
Applications of Differential Calculus in real life
 

Recently uploaded

Governing Equations for Fundamental Aerodynamics_Anderson2010.pdf
Governing Equations for Fundamental Aerodynamics_Anderson2010.pdfGoverning Equations for Fundamental Aerodynamics_Anderson2010.pdf
Governing Equations for Fundamental Aerodynamics_Anderson2010.pdf
WENKENLI1
 
Top 10 Oil and Gas Projects in Saudi Arabia 2024.pdf
Top 10 Oil and Gas Projects in Saudi Arabia 2024.pdfTop 10 Oil and Gas Projects in Saudi Arabia 2024.pdf
Top 10 Oil and Gas Projects in Saudi Arabia 2024.pdf
Teleport Manpower Consultant
 
Cosmetic shop management system project report.pdf
Cosmetic shop management system project report.pdfCosmetic shop management system project report.pdf
Cosmetic shop management system project report.pdf
Kamal Acharya
 
space technology lecture notes on satellite
space technology lecture notes on satellitespace technology lecture notes on satellite
space technology lecture notes on satellite
ongomchris
 
Fundamentals of Electric Drives and its applications.pptx
Fundamentals of Electric Drives and its applications.pptxFundamentals of Electric Drives and its applications.pptx
Fundamentals of Electric Drives and its applications.pptx
manasideore6
 
AP LAB PPT.pdf ap lab ppt no title specific
AP LAB PPT.pdf ap lab ppt no title specificAP LAB PPT.pdf ap lab ppt no title specific
AP LAB PPT.pdf ap lab ppt no title specific
BrazilAccount1
 
CFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptx
CFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptxCFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptx
CFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptx
R&R Consult
 
Hybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdf
Hybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdfHybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdf
Hybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdf
fxintegritypublishin
 
NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...
NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...
NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...
Amil Baba Dawood bangali
 
DESIGN A COTTON SEED SEPARATION MACHINE.docx
DESIGN A COTTON SEED SEPARATION MACHINE.docxDESIGN A COTTON SEED SEPARATION MACHINE.docx
DESIGN A COTTON SEED SEPARATION MACHINE.docx
FluxPrime1
 
power quality voltage fluctuation UNIT - I.pptx
power quality voltage fluctuation UNIT - I.pptxpower quality voltage fluctuation UNIT - I.pptx
power quality voltage fluctuation UNIT - I.pptx
ViniHema
 
ethical hacking-mobile hacking methods.ppt
ethical hacking-mobile hacking methods.pptethical hacking-mobile hacking methods.ppt
ethical hacking-mobile hacking methods.ppt
Jayaprasanna4
 
Architectural Portfolio Sean Lockwood
Architectural Portfolio Sean LockwoodArchitectural Portfolio Sean Lockwood
Architectural Portfolio Sean Lockwood
seandesed
 
Planning Of Procurement o different goods and services
Planning Of Procurement o different goods and servicesPlanning Of Procurement o different goods and services
Planning Of Procurement o different goods and services
JoytuBarua2
 
Investor-Presentation-Q1FY2024 investor presentation document.pptx
Investor-Presentation-Q1FY2024 investor presentation document.pptxInvestor-Presentation-Q1FY2024 investor presentation document.pptx
Investor-Presentation-Q1FY2024 investor presentation document.pptx
AmarGB2
 
The Benefits and Techniques of Trenchless Pipe Repair.pdf
The Benefits and Techniques of Trenchless Pipe Repair.pdfThe Benefits and Techniques of Trenchless Pipe Repair.pdf
The Benefits and Techniques of Trenchless Pipe Repair.pdf
Pipe Restoration Solutions
 
WATER CRISIS and its solutions-pptx 1234
WATER CRISIS and its solutions-pptx 1234WATER CRISIS and its solutions-pptx 1234
WATER CRISIS and its solutions-pptx 1234
AafreenAbuthahir2
 
在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样
在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样
在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样
obonagu
 
J.Yang, ICLR 2024, MLILAB, KAIST AI.pdf
J.Yang,  ICLR 2024, MLILAB, KAIST AI.pdfJ.Yang,  ICLR 2024, MLILAB, KAIST AI.pdf
J.Yang, ICLR 2024, MLILAB, KAIST AI.pdf
MLILAB
 
block diagram and signal flow graph representation
block diagram and signal flow graph representationblock diagram and signal flow graph representation
block diagram and signal flow graph representation
Divya Somashekar
 

Recently uploaded (20)

Governing Equations for Fundamental Aerodynamics_Anderson2010.pdf
Governing Equations for Fundamental Aerodynamics_Anderson2010.pdfGoverning Equations for Fundamental Aerodynamics_Anderson2010.pdf
Governing Equations for Fundamental Aerodynamics_Anderson2010.pdf
 
Top 10 Oil and Gas Projects in Saudi Arabia 2024.pdf
Top 10 Oil and Gas Projects in Saudi Arabia 2024.pdfTop 10 Oil and Gas Projects in Saudi Arabia 2024.pdf
Top 10 Oil and Gas Projects in Saudi Arabia 2024.pdf
 
Cosmetic shop management system project report.pdf
Cosmetic shop management system project report.pdfCosmetic shop management system project report.pdf
Cosmetic shop management system project report.pdf
 
space technology lecture notes on satellite
space technology lecture notes on satellitespace technology lecture notes on satellite
space technology lecture notes on satellite
 
Fundamentals of Electric Drives and its applications.pptx
Fundamentals of Electric Drives and its applications.pptxFundamentals of Electric Drives and its applications.pptx
Fundamentals of Electric Drives and its applications.pptx
 
AP LAB PPT.pdf ap lab ppt no title specific
AP LAB PPT.pdf ap lab ppt no title specificAP LAB PPT.pdf ap lab ppt no title specific
AP LAB PPT.pdf ap lab ppt no title specific
 
CFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptx
CFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptxCFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptx
CFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptx
 
Hybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdf
Hybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdfHybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdf
Hybrid optimization of pumped hydro system and solar- Engr. Abdul-Azeez.pdf
 
NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...
NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...
NO1 Uk best vashikaran specialist in delhi vashikaran baba near me online vas...
 
DESIGN A COTTON SEED SEPARATION MACHINE.docx
DESIGN A COTTON SEED SEPARATION MACHINE.docxDESIGN A COTTON SEED SEPARATION MACHINE.docx
DESIGN A COTTON SEED SEPARATION MACHINE.docx
 
power quality voltage fluctuation UNIT - I.pptx
power quality voltage fluctuation UNIT - I.pptxpower quality voltage fluctuation UNIT - I.pptx
power quality voltage fluctuation UNIT - I.pptx
 
ethical hacking-mobile hacking methods.ppt
ethical hacking-mobile hacking methods.pptethical hacking-mobile hacking methods.ppt
ethical hacking-mobile hacking methods.ppt
 
Architectural Portfolio Sean Lockwood
Architectural Portfolio Sean LockwoodArchitectural Portfolio Sean Lockwood
Architectural Portfolio Sean Lockwood
 
Planning Of Procurement o different goods and services
Planning Of Procurement o different goods and servicesPlanning Of Procurement o different goods and services
Planning Of Procurement o different goods and services
 
Investor-Presentation-Q1FY2024 investor presentation document.pptx
Investor-Presentation-Q1FY2024 investor presentation document.pptxInvestor-Presentation-Q1FY2024 investor presentation document.pptx
Investor-Presentation-Q1FY2024 investor presentation document.pptx
 
The Benefits and Techniques of Trenchless Pipe Repair.pdf
The Benefits and Techniques of Trenchless Pipe Repair.pdfThe Benefits and Techniques of Trenchless Pipe Repair.pdf
The Benefits and Techniques of Trenchless Pipe Repair.pdf
 
WATER CRISIS and its solutions-pptx 1234
WATER CRISIS and its solutions-pptx 1234WATER CRISIS and its solutions-pptx 1234
WATER CRISIS and its solutions-pptx 1234
 
在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样
在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样
在线办理(ANU毕业证书)澳洲国立大学毕业证录取通知书一模一样
 
J.Yang, ICLR 2024, MLILAB, KAIST AI.pdf
J.Yang,  ICLR 2024, MLILAB, KAIST AI.pdfJ.Yang,  ICLR 2024, MLILAB, KAIST AI.pdf
J.Yang, ICLR 2024, MLILAB, KAIST AI.pdf
 
block diagram and signal flow graph representation
block diagram and signal flow graph representationblock diagram and signal flow graph representation
block diagram and signal flow graph representation
 

Triple Integral

  • 1.
  • 2. Triple Integral Definition of the Triple Integral Theorem for Evaluating Triple Integrals Theory  Meaning Rules For Solving Polar ( cylindrical ) Coordinates Examples References
  • 3. Let f(x,y,z) be a continuous function of three variables defined over a solid Q. Then the triple integral over Q is defined as ∭ 𝑓( 𝑥, 𝑦, 𝑧) = 𝑙𝑖𝑚 ∑ 𝑓( 𝑥, 𝑦, 𝑧)∆𝑥∆𝑦∆𝑧 𝑄 where the sum is taken over the rectangular solids included in the solid Q and lim is taken to mean the limit as the side lengths of the rectangular solid. DefinitionoftheTripleIntegral Let f(x,y,z) be a continuous function over a solid Q defined by a < x < b h1(x) < y < h2(x) g1(x,y) < z < g2(x,y) Then the triple integral is equal to the triple iterated integral. TheoremforEvaluatingTripleIntegrals ∭ f(x, y, z) = ∫ ∫ ∫ f(x, y,z, )dz dy dx g2(x,y) g1(x,y) h2(x) h1(x) b a𝑄
  • 4.  As the name implies, triple integrals are 3 successive integrations, used to calculate a volume, or to integrate in a 4th dimension, over 3 other independent dimensions. Examples: Theory ∭ 𝑓 ( 𝑥, 𝑦, 𝑧) 𝑑𝑉 𝑉 0 ∫ ∫ 1 3X−2 0 5 1 ∫ (2X + eyz)dz dy dx COS(X+Y) SIN(X+Y) ∫ 1 2𝜋 0 ∫ 1 2 0 ∫ 𝑟 𝑑𝑧 𝑑𝑟 𝑑𝜃 3 −3  To understand triple integrals, it is extremely important to have an understanding of double integrals, coordinate geometry in 3 dimensions, and polar (cylindrical) coordinates. Sums of triple integrals are based on these topics and cannot be solved without this prior knowledge.  Just as a single integral over a curve represents an area (2D), and a double integral over a curve represents a volume (3D), a triple integral represents a summation in a hypothetical 4th dimension. To understand this, imagine a slightly different scenario, where the first 3 dimensions are space, space, and time, and that the fourth dimension is the third space dimension: suppose you have an integral of z where z is a function of x, y, and t, and x and y are also functions of t. Integrating z with respect to x and y gives us the volume as a function of t. If we plug in a value for t, this gives us the numerical volume at a particular instance of time. Meaning
  • 5.  However, as the volume is a function of t, it changes with respect to time. Thus, if we integrate this result with respect to t, we are adding up all the different volumes over a period of time. For example, imagine a balloon that is being inflated. At any particular instant of time, we can use a double integral to calculate its volume. However, if we wanted to sum up all the volumes over the entire inflation process, we must use a triple integral as described above. Meaning(Contd.)  Triple Integrals can also be used to represent a volume, in the same way that a double integral can be used to represent an area. In the triple integral ∫ ∫ ∫ 𝑓 ( 𝑥, 𝑦, 𝑧 ) 𝑑𝑧 𝑑𝑦 𝑑𝑥 𝑧 0 𝑏 𝑎 𝑑 𝑐 If 𝑓( 𝑥, 𝑦, 𝑧, ) = 1 then this triple integral is the same as ∫ ∫ 𝑧 ( 𝑥, 𝑦 ) 𝑑𝑦 𝑑𝑥 𝑏 𝑎 𝑑 𝑐 Which is simply the volume under the surface represented by 𝑧 ( 𝑥, 𝑦 ) .
  • 6. RulesForSolving  In general, if you are evaluating a triple integral of f( x,y,z ) over a volume V, by properly choosing the limits, you can integrate with respect to the 3 variables in any order. For example, if V represents a rectangular box, then for x, y, and z, the limits of integration will all be constants and the order does not matter at all. ∫ ∫ ∫ 𝑓 𝑑𝑧 𝑑𝑦 𝑑𝑥 = ∫ ∫ ∫ 𝑓 𝑑𝑥 𝑑𝑧 𝑑𝑦 = ⋯ 𝑓 𝑒 𝑏 𝑎 𝑑 𝑐 𝑏 𝑎 𝑑 𝑐 𝑓 𝑒 and so on, for 6 different possible orders of integration. Now consider the case where you want to find the triple integral ∭ 𝑓 ( 𝑥, 𝑦, 𝑧 ) 𝑑𝑉 𝑉 0 where V is the volume under the plane 𝑧+2𝑥+3𝑦=6, in the first quadrant. Since V is in the first quadrant, it is bounded by the 3 planes 𝑥=0,𝑦=0,𝑧=0 in addition to the plane whose equation is given above. Clearly, the shape of V is a tetrahedron with the vertices (3,0,0), (0,2,0), (0,0,6), and (0,0,0).
  • 7. One way to set up the integral is to first consider the z direction. In this direction we enter through 𝑧=0 and leave through 𝑧=6−2𝑥−3𝑦. If we do this first, then we can consider the x or y direction next. If y, we enter through 𝑦=0, and leave through 𝑦 = − 2 3 𝑥 + 2. Thus, x must be given the limits 0 to 3, and our triple integral is: ∫ ∫ ∫ 𝑓 ( 𝑥, 𝑦, 𝑧) 𝑑𝑧 𝑑𝑦 𝑑𝑥 6−2𝑥−3𝑦 0 − 2 3 𝑥+2 0 3 0 Consider the same volume, but now first we will go through in the x direction. In this direction we enter through x=0 and leave through 𝑥= 1 2 (6−𝑧−3𝑦). If we do this first, then we can consider the z or y direction next. If y, we enter through 𝑦=0, and leave through 𝑦=− 1 3 𝑧+2, and z must be from 0 to 6. Thus the integral would be ∫ ∫ ∫ 𝑓 ( 𝑥, 𝑦, 𝑧 ) 𝑑𝑥 𝑑𝑦 𝑑𝑧 1 2 (6−𝑧−3𝑦) 0 − 1 3 𝑧+2 0 6 0 Both these integrals are correct and either one can be used to solve the sum and obtain the same value. It is important to see that choosing the order of integration depends on how the limits are chosen. However, this is entirely independent of the function 𝑓(𝑥,𝑦,𝑧). In the first case, z must be integrated first, since the limits were chosen such that z is dependent on (x,y). After this, since y is chosen to be dependent on x, y is integrated next. Lastly, x as the most independent variable is integrated. It is important to note that the third (outermost) integral MUST always have limits of integration that are constants, and the result should be a number. If any variables are surviving after the integral is evaluated, most probably you have made a mistake somewhere.
  • 8. Polar(cylindrical)Coordinates Triple integrals can also be used with polar coordinates in the exact same way to calculate a volume, or to integrate over a volume. For example: ∫ ∫ ∫ 𝑟 𝑑𝑧 𝑑𝑟 𝑑𝜃 3 −3 2 0 2𝜋 0 is the triple integral used to calculate the volume of a cylinder of height 6 and radius 2. With polar coordinates, usually the easiest order of integration is 𝑧, then 𝑟 then 𝜃 as shown above, though it is not necessary to do it in this order. NOTE: It is very important to remember that in polar and cylindrical coordinates, there is an extra 𝒓 in the integral, just like in double integrals. It is very easy to forget this 𝒓 which will lead to a wrong answer.
  • 9. 1. Integrate the function 𝑓(𝑥,𝑦,𝑧)=𝑥𝑦 over the volume enclose by the planes 𝑧=𝑥+𝑦 and 𝑧=0, and between the surfaces 𝑦=𝑥2 and 𝑥=𝑦2. SOLUTION: Since z is expressed as a function of (x,y), we should integrate in the z direction first. After this we consider the xy-plane. The two curves meet at (0,0) and (1,1). We can integrate in x or y first. If we choose y, we can see that the region begins at 𝑦=𝑥2 and ends at 𝑦=√𝑥, and so x is between 0 and 1. Thus the integral is: ∫ ∫ ∫ f(x, y, z)dz dy dx x+y 0 √x2 x2 1 0 ∫ ∫ 𝑥𝑦 ( 𝑧 = 𝑥 + 𝑦 𝑧 = 0 [ 𝑧]) 𝑑𝑦𝑑𝑥 √ 𝑥 𝑥2 1 0 ∫ ∫ xy(x + y)dy dx √x x2 1 0 ∫ ∫ ( 𝑥2 𝑦 + 𝑦2 𝑥) 𝑑𝑦 𝑑𝑥 √ 𝑥 𝑥2 1 0 ∫ 𝑦 = √ 𝑥 𝑦 = 𝑥2 ( 𝑥2 𝑦2 2 + 𝑦3 𝑥 3 ) 𝑑𝑥 1 0 1 2 ∫ ( 𝑥2 √ 𝑥 2 − 𝑥2( 𝑥2) 2) 𝑑𝑥 + 1 3 ∫ (√ 𝑥 3 𝑥 − ( 𝑥2)3 𝑥)𝑑𝑥 1 0 1 0 1 2 ∫ ( 𝑥3 − 𝑥6) 𝑑𝑥 + 1 3 ∫ ( 𝑥 5 2 − 𝑥7) 𝑑𝑥 1 0 1 0 1 2 ( 1 4 − 1 7 ) + 1 3 ( 2 7 − 1 8 ) = 3 28 Examples
  • 10. 2. In the following integral, exchange the order of integrationof y and z: ∫ ∫ ∫ f(x, y,z)dz dy dx 1−y 0 1 √x 1 0 SOLUTION: With a problem like this, it helps to draw the figure enclose by the surfaces. From the integrals, it can be seen that z enters the volume at 𝑧=0 and leaves through the plane 𝑧=1−𝑦. In the 𝑥𝑦 plane, 𝑦 enters through 𝑦=√ 𝑥 and leaves through 𝑦=1. These 2 conditions alone are enough to draw the figure and see that 0≤𝑥≤1. The shape is like a tetrahedron with the vertices A(0,0,0), B(0,0,1), C(1,1,0), and D(0,1,0), but with a curved surface between vertices A, B, C. Rewriting the equation of the plane as 𝑦=1−𝑧, and looking at this figure, clearly, √ 𝑥≤𝑦≤1−𝑧. Consider the projection of this surface in the 𝑧𝑥 plane. It is a 3-sided figure bounded by 𝑥=0,𝑧=0,and 𝑧=1−√ 𝑥. Again, it can be seen that these conditions are sufficient to obtain the limits of x as 0≤𝑥≤1. Thus, the integral is: ∫ ∫ ∫ f(x, y,z)dy dz dx 1−z √x 1−√x 0 1 0
  • 11. 3. Evaluate ∭ 𝐸 xdV where E is enclosed by 𝑧=0,𝑧=𝑥+𝑦+5,𝑥2+𝑦2=4 and 𝑥2+𝑦2=9. SOLUTION: We will use cylindrical coordinates to easily solve this sum. Converting the given outer limits of E we get: 𝑧=0,𝑧=𝑟cosθ+𝑟sinθ+5,𝑟=2 and 𝑟=3. Since there is no limitation on the values of θ, we assume it has the values of 0 to 2π. This is also in accordance with the diagram which is obtained by drawing these surfaces. Also, we substitute 𝑥=𝑟cosθ in the argument of the integral. Thus the integral is: ∫ ∫ ∫ (𝑟 cos 𝜃)𝑟 𝑑𝑧 𝑑𝑟 𝑑𝜃 𝑟𝑐𝑜𝑠 𝜃+𝑟 sin 𝜃+5 0 3 2 2𝜋 0 = ∫ ∫ (𝑟2 cos 𝜃) (𝑟 cos 𝜃 + 𝑟 sin 𝜃 + 5) 𝑑𝑟 𝑑𝜃 3 2 2𝜋 0 ∫ 𝑟 = 3 𝑟 = 2 [ 𝑟4 4 𝑐𝑜𝑠2 𝜃 + 𝑟4 4 cos 𝜃 sin 𝜃 + 5 3 𝑟3 cos 𝜃] 2𝜋 0 𝑑𝜃 ∫ [ 65 8 (1 + cos 2𝜃) + 65 8 𝑠𝑖𝑛 (2𝜃) + 95 3 cos 𝜃] 2𝜋 0 𝑑𝜃 = 65 8 (2𝜋 + 0 − 1 2 + 0 − 0 + 1 2 ) + 95 3 (0) = 65𝜋 4
  • 12. References  Calculus – Sixth Edition James Stewart  Rohit Agarwal – Math Scholar at Academic Resource Center  Illinois Institute of Technology  WIKIPEDIA