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multivariable calculus
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Multivariable calculus (also known as multivariate calculus) is the extension of calculus in one variable to calculus with functions of several variables: the differentiation and integration of functions involving multiple variables (multivariate), rather than just one.
Multivariable calculus may be thought of as an elementary part of calculus on Euclidean space. The special case of calculus in three dimensional space is often called vector calculus.
Introduction
In single-variable calculus, operations like differentiation and integration are made to functions of a single variable. In multivariate calculus, it is required to generalize these to multiple variables, and the domain is therefore multi-dimensional. Care is therefore required in these generalizations, because of two key differences between 1D and higher dimensional spaces:
There are infinite ways to approach a single point in higher dimensions, as opposed to two (from the positive and negative direction) in 1D;
There are multiple extended objects associated with the dimension; for example, for a 1D function, it must be represented as a curve on the 2D Cartesian plane, but a function with two variables is a surface in 3D, while curves can also live in 3D space.
The consequence of the first difference is the difference in the definition of the limit and differentiation. Directional limits and derivatives define the limit and differential along a 1D parametrized curve, reducing the problem to the 1D case. Further higher-dimensional objects can be constructed from these operators.
The consequence of the second difference is the existence of multiple types of integration, including line integrals, surface integrals and volume integrals. Due to the non-uniqueness of these integrals, an antiderivative or indefinite integral cannot be properly defined.
Limits
A study of limits and continuity in multivariable calculus yields many counterintuitive results not demonstrated by single-variable functions.
A limit along a path may be defined by considering a parametrised path
s
(
t
)
:
R
→
R
n
{\displaystyle s(t):\mathbb {R} \to \mathbb {R} ^{n}}
in n-dimensional Euclidean space. Any function
f
(
x
→
)
:
R
n
→
R
m
{\displaystyle f({\overrightarrow {x}}):\mathbb {R} ^{n}\to \mathbb {R} ^{m}}
can then be projected on the path as a 1D function
f
(
s
(
t
)
)
{\displaystyle f(s(t))}
. The limit of
f
{\displaystyle f}
to the point
s
(
t
0
)
{\displaystyle s(t_{0})}
along the path
s
(
t
)
{\displaystyle s(t)}
can hence be defined as
Note that the value of this limit can be dependent on the form of
s
(
t
)
{\displaystyle s(t)}
, i.e. the path chosen, not just the point which the limit approaches.: 19–22 For example, consider the function
f
(
x
,
y
)
=
x
2
y
x
4
+
y
2
.
{\displaystyle f(x,y)={\frac {x^{2}y}{x^{4}+y^{2}}}.}
If the point
(
0
,
0
)
{\displaystyle (0,0)}
is approached through the line
y
=
k
x
{\displaystyle y=kx}
, or in parametric form:
Then the limit along the path will be:
On the other hand, if the path
y
=
±
x
2
{\displaystyle y=\pm x^{2}}
(or parametrically,
x
(
t
)
=
t
,
y
(
t
)
=
±
t
2
{\displaystyle x(t)=t,\,y(t)=\pm t^{2}}
) is chosen, then the limit becomes:
Since taking different paths towards the same point yields different values, a general limit at the point
(
0
,
0
)
{\displaystyle (0,0)}
cannot be defined for the function.
A general limit can be defined if the limits to a point along all possible paths converge to the same value, i.e. we say for a function
f
:
R
n
→
R
m
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} ^{m}}
that the limit of
f
{\displaystyle f}
to some point
x
0
∈
R
n
{\displaystyle x_{0}\in \mathbb {R} ^{n}}
is L, if and only if
for all continuous functions
s
(
t
)
:
R
→
R
n
{\displaystyle s(t):\mathbb {R} \to \mathbb {R} ^{n}}
such that
s
(
t
0
)
=
x
0
{\displaystyle s(t_{0})=x_{0}}
.
= Continuity
=From the concept of limit along a path, we can then derive the definition for multivariate continuity in the same manner, that is: we say for a function
f
:
R
n
→
R
m
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} ^{m}}
that
f
{\displaystyle f}
is continuous at the point
x
0
{\displaystyle x_{0}}
, if and only if
for all continuous functions
s
(
t
)
:
R
→
R
n
{\displaystyle s(t):\mathbb {R} \to \mathbb {R} ^{n}}
such that
s
(
t
0
)
=
x
0
{\displaystyle s(t_{0})=x_{0}}
.
As with limits, being continuous along one path
s
(
t
)
{\displaystyle s(t)}
does not imply multivariate continuity.
Continuity in each argument not being sufficient for multivariate continuity can also be seen from the following example.: 17–19 For example, for a real-valued function
f
:
R
2
→
R
{\displaystyle f:\mathbb {R} ^{2}\to \mathbb {R} }
with two real-valued parameters,
f
(
x
,
y
)
{\displaystyle f(x,y)}
, continuity of
f
{\displaystyle f}
in
x
{\displaystyle x}
for fixed
y
{\displaystyle y}
and continuity of
f
{\displaystyle f}
in
y
{\displaystyle y}
for fixed
x
{\displaystyle x}
does not imply continuity of
f
{\displaystyle f}
.
Consider
f
(
x
,
y
)
=
{
y
x
−
y
if
0
≤
y
<
x
≤
1
x
y
−
x
if
0
≤
x
<
y
≤
1
1
−
x
if
0
<
x
=
y
0
everywhere else
.
{\displaystyle f(x,y)={\begin{cases}{\frac {y}{x}}-y&{\text{if}}\quad 0\leq y
It is easy to verify that this function is zero by definition on the boundary and outside of the quadrangle
(
0
,
1
)
×
(
0
,
1
)
{\displaystyle (0,1)\times (0,1)}
. Furthermore, the functions defined for constant
x
{\displaystyle x}
and
y
{\displaystyle y}
and
0
≤
a
≤
1
{\displaystyle 0\leq a\leq 1}
by
g
a
(
x
)
=
f
(
x
,
a
)
{\displaystyle g_{a}(x)=f(x,a)\quad }
and
h
a
(
y
)
=
f
(
a
,
y
)
{\displaystyle \quad h_{a}(y)=f(a,y)\quad }
are continuous. Specifically,
g
0
(
x
)
=
f
(
x
,
0
)
=
h
0
(
0
,
y
)
=
f
(
0
,
y
)
=
0
{\displaystyle g_{0}(x)=f(x,0)=h_{0}(0,y)=f(0,y)=0}
for all x and y. Therefore,
f
(
0
,
0
)
=
0
{\displaystyle f(0,0)=0}
and moreover, along the coordinate axes,
lim
x
→
0
f
(
x
,
0
)
=
0
{\displaystyle \lim _{x\to 0}f(x,0)=0}
and
lim
y
→
0
f
(
0
,
y
)
=
0
{\displaystyle \lim _{y\to 0}f(0,y)=0}
. Therefore the function is continuous along both individual arguments.
However, consider the parametric path
x
(
t
)
=
t
,
y
(
t
)
=
t
{\displaystyle x(t)=t,\,y(t)=t}
. The parametric function becomes
Therefore,
It is hence clear that the function is not multivariate continuous, despite being continuous in both coordinates.
= Theorems regarding multivariate limits and continuity
=All properties of linearity and superposition from single-variable calculus carry over to multivariate calculus.
Composition: If
f
:
R
n
→
R
m
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} ^{m}}
and
g
:
R
m
→
R
p
{\displaystyle g:\mathbb {R} ^{m}\to \mathbb {R} ^{p}}
are both multivariate continuous functions at the points
x
0
∈
R
n
{\displaystyle x_{0}\in \mathbb {R} ^{n}}
and
f
(
x
0
)
∈
R
m
{\displaystyle f(x_{0})\in \mathbb {R} ^{m}}
respectively, then
g
∘
f
:
R
n
→
R
p
{\displaystyle g\circ f:\mathbb {R} ^{n}\to \mathbb {R} ^{p}}
is also a multivariate continuous function at the point
x
0
{\displaystyle x_{0}}
.
Multiplication: If
f
:
R
n
→
R
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} }
and
g
:
R
n
→
R
{\displaystyle g:\mathbb {R} ^{n}\to \mathbb {R} }
are both continuous functions at the point
x
0
∈
R
n
{\displaystyle x_{0}\in \mathbb {R} ^{n}}
, then
f
g
:
R
n
→
R
{\displaystyle fg:\mathbb {R} ^{n}\to \mathbb {R} }
is continuous at
x
0
{\displaystyle x_{0}}
, and
f
/
g
:
R
n
→
R
{\displaystyle f/g:\mathbb {R} ^{n}\to \mathbb {R} }
is also continuous at
x
0
{\displaystyle x_{0}}
provided that
g
(
x
0
)
≠
0
{\displaystyle g(x_{0})\neq 0}
.
If
f
:
R
n
→
R
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} }
is a continuous function at point
x
0
∈
R
n
{\displaystyle x_{0}\in \mathbb {R} ^{n}}
, then
|
f
|
{\displaystyle |f|}
is also continuous at the same point.
If
f
:
R
n
→
R
m
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} ^{m}}
is Lipschitz continuous (with the appropriate normed spaces as needed) in the neighbourhood of the point
x
0
∈
R
n
{\displaystyle x_{0}\in \mathbb {R} ^{n}}
, then
f
{\displaystyle f}
is multivariate continuous at
x
0
{\displaystyle x_{0}}
.
Differentiation
= Directional derivative
=The derivative of a single-variable function is defined as
Using the extension of limits discussed above, one can then extend the definition of the derivative to a scalar-valued function
f
:
R
n
→
R
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} }
along some path
s
(
t
)
:
R
→
R
n
{\displaystyle s(t):\mathbb {R} \to \mathbb {R} ^{n}}
:
Unlike limits, for which the value depends on the exact form of the path
s
(
t
)
{\displaystyle s(t)}
, it can be shown that the derivative along the path depends only on the tangent vector of the path at
s
(
t
0
)
{\displaystyle s(t_{0})}
, i.e.
s
′
(
t
0
)
{\displaystyle s'(t_{0})}
, provided that
f
{\displaystyle f}
is Lipschitz continuous at
s
(
t
0
)
{\displaystyle s(t_{0})}
, and that the limit exits for at least one such path.
It is therefore possible to generate the definition of the directional derivative as follows: The directional derivative of a scalar-valued function
f
:
R
n
→
R
{\displaystyle f:\mathbb {R} ^{n}\to \mathbb {R} }
along the unit vector
u
^
{\displaystyle {\hat {\mathbf {u}}}}
at some point
x
0
∈
R
n
{\displaystyle x_{0}\in \mathbb {R} ^{n}}
is
or, when expressed in terms of ordinary differentiation,
which is a well defined expression because
f
(
x
0
+
u
^
t
)
{\displaystyle f(x_{0}+{\hat {\mathbf {u}}}t)}
is a scalar function with one variable in
t
{\displaystyle t}
.
It is not possible to define a unique scalar derivative without a direction; it is clear for example that
∇
u
^
f
(
x
0
)
=
−
∇
−
u
^
f
(
x
0
)
{\displaystyle \nabla _{\hat {\mathbf {u}}}f(x_{0})=-\nabla _{-{\hat {\mathbf {u}}}}f(x_{0})}
. It is also possible for directional derivatives to exist for some directions but not for others.
= Partial derivative
=The partial derivative generalizes the notion of the derivative to higher dimensions. A partial derivative of a multivariable function is a derivative with respect to one variable with all other variables held constant.: 26ff
A partial derivative may be thought of as the directional derivative of the function along a coordinate axis.
Partial derivatives may be combined in interesting ways to create more complicated expressions of the derivative. In vector calculus, the del operator (
∇
{\displaystyle \nabla }
) is used to define the concepts of gradient, divergence, and curl in terms of partial derivatives. A matrix of partial derivatives, the Jacobian matrix, may be used to represent the derivative of a function between two spaces of arbitrary dimension. The derivative can thus be understood as a linear transformation which directly varies from point to point in the domain of the function.
Differential equations containing partial derivatives are called partial differential equations or PDEs. These equations are generally more difficult to solve than ordinary differential equations, which contain derivatives with respect to only one variable.: 654ff
Multiple integration
The multiple integral extends the concept of the integral to functions of any number of variables. Double and triple integrals may be used to calculate areas and volumes of regions in the plane and in space. Fubini's theorem guarantees that a multiple integral may be evaluated as a repeated integral or iterated integral as long as the integrand is continuous throughout the domain of integration.: 367ff
The surface integral and the line integral are used to integrate over curved manifolds such as surfaces and curves.
= Fundamental theorem of calculus in multiple dimensions
=In single-variable calculus, the fundamental theorem of calculus establishes a link between the derivative and the integral. The link between the derivative and the integral in multivariable calculus is embodied by the integral theorems of vector calculus:: 543ff
Gradient theorem
Stokes' theorem
Divergence theorem
Green's theorem.
In a more advanced study of multivariable calculus, it is seen that these four theorems are specific incarnations of a more general theorem, the generalized Stokes' theorem, which applies to the integration of differential forms over manifolds.
Applications and uses
Techniques of multivariable calculus are used to study many objects of interest in the material world. In particular,
Multivariable calculus can be applied to analyze deterministic systems that have multiple degrees of freedom. Functions with independent variables corresponding to each of the degrees of freedom are often used to model these systems, and multivariable calculus provides tools for characterizing the system dynamics.
Multivariate calculus is used in the optimal control of continuous time dynamic systems. It is used in regression analysis to derive formulas for estimating relationships among various sets of empirical data.
Multivariable calculus is used in many fields of natural and social science and engineering to model and study high-dimensional systems that exhibit deterministic behavior. In economics, for example, consumer choice over a variety of goods, and producer choice over various inputs to use and outputs to produce, are modeled with multivariate calculus.
Non-deterministic, or stochastic systems can be studied using a different kind of mathematics, such as stochastic calculus.
See also
List of multivariable calculus topics
Multivariate statistics
References
External links
UC Berkeley video lectures on Multivariable Calculus, Fall 2009, Professor Edward Frenkel
MIT video lectures on Multivariable Calculus, Fall 2007
Multivariable Calculus: A free online textbook by George Cain and James Herod
Multivariable Calculus Online: A free online textbook by Jeff Knisley
Multivariable Calculus – A Very Quick Review, Prof. Blair Perot, University of Massachusetts Amherst
Multivariable Calculus, Online text by Dr. Jerry Shurman
Kata Kunci Pencarian: multivariable calculus
multivariable calculus
Daftar Isi
Multivariable calculus - Wikipedia
Multivariable calculus (also known as multivariate calculus) is the extension of calculus in one variable to calculus with functions of several variables: the differentiation and integration of functions involving multiple variables (multivariate), rather than just one.
Multivariable Calculus - Khan Academy
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Multivariable Calculus | Mathematics | MIT OpenCourseWare
This course covers differential, integral and vector calculus for functions of more than one variable. These mathematical tools and methods are used extensively in the physical sciences, engineering, economics and computer graphics.
12.1: Introduction to Multivariable Functions
Dec 29, 2020 · Let D be a subset of R2. A function f of two variables is a rule that assigns each pair (x, y) in D a value z = f(x, y) in R. D is the domain of f; the set of all outputs of f is the range. Let z = f(x, y) = x2 − y. Evaluate f(1, 2), f(2, 1), and f(− 2, 4); find the domain and range of f. Solution. Using the definition f(x, y) = x2 − y, we have:
Syllabus | Multivariable Calculus - MIT OpenCourseWare
In multivariable calculus we study functions of two or more independent variables, e.g., z=f(x, y) or w=f(x, y, z) . These functions are interesting in their own right, but they are also essential for describing the physical world.
Multivariable Calculus | Mathematics | MIT OpenCourseWare
This course covers vector and multi-variable calculus. It is the second semester in the freshman calculus sequence. Topics include vectors and matrices, partial derivatives, double and triple integrals, and vector calculus in 2 and 3-space.
Multivariable Calculus - Harvard Division of Continuing Education ...
This course covers the following topics: calculus of functions of several variables; vectors and vector-valued functions; parameterized curves and surfaces; vector fields; partial derivatives and gradients; optimization; method of Lagrange multipliers; integration over regions in R 2 and R 3; integration over curves and surfaces; Green's theorem...
Multivariable Calculus, Online Video Course: Wolfram U
Multivariable calculus extends the notions of limits, derivatives and integrals to higher dimensions. It also considers constrained and unconstrained optimization problems and explores the three great theorems of multivariable calculus: Green's theorem, Stokes' theorem and …
Multivariable Calculus - Open Textbook Library
Dec 19, 2019 · This book covers the standard material for a one-semester course in multivariable calculus. The topics include curves, differentiability and partial derivatives, multiple integrals, vector fields, line and surface integrals, and the theorems of Green, Stokes, and Gauss.
Multivariable Calculus | Important Topics in Multivariate Calculus
In Mathematics, multivariable calculus or multivariate calculus is an extension of calculus in one variable with functions of several variables. The differentiation and integration process involves multiple variables, rather than once.