Vector



A vector is formally defined as an element of a vector space. In the commonly encountered vector space (i.e., Euclidean n-space),
a vector is given by
coordinates and can be specified as
. Vectors are sometimes referred to by the number
of coordinates they have, so a 2-dimensional vector
is often
called a two-vector, an
-dimensional vector is often called an
n-vector, and so on.
Vectors can be added together (vector addition), subtracted (vector subtraction) and multiplied by scalars (scalar multiplication). Vector multiplication is not uniquely defined, but a number of different types of products, such as the dot product, cross product, and tensor direct product can be defined for pairs of vectors.
A vector from a point to a point
is denoted
, and a vector
may be denoted
, or more commonly,
. The point
is often called the "tail" of the vector, and
is called the vector's "head." A vector with unit
length is called a unit vector and is denoted using
a hat,
.
When written out componentwise, the notation generally refers
to
. On the other hand, when written
with a subscript, the notation
(or
) generally refers
to
.
An arbitrary vector may be converted to a unit vector by dividing by its norm (i.e., length; i.e., magnitude),
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(1)
|
giving
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(2)
|
A zero vector, denoted , is a vector of
length 0, and thus has all components equal to zero.
Since vectors remain unchanged under translation, it is often convenient to consider the tail as located at the
origin when, for example, defining vector addition
and scalar multiplication.
A vector may also be defined as a set of numbers
, ...,
that transform
according to the rule
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(3)
|
where Einstein summation notation has been used,
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(4)
|
are constants (corresponding to the direction cosines), with partial derivatives taken with respect to the original and transformed coordinate
axes, and , ...,
(Arfken 1985, p. 10).
This makes a vector a tensor of tensor
rank one. A vector with
components in called an
-vector, and a scalar may therefore be thought of as a 1-vector (or a 0-tensor rank tensor). Vectors
are invariant under translation, and they reverse
sign upon inversion. Objects that resemble vectors but do not reverse sign upon inversion
are known as pseudovectors. To distinguish vectors
from pseudovectors, the former are sometimes called
polar vectors.
A vector is represented in Mathematica as a list of numbers a1, a2, ..., an
. Vector addition is then
simply written using a plus sign, e.g.,
a1, a2,
..., an
+
b1, b2,
..., bn
, and scalar
multiplication is indicated by placing a scalar next to a vector (with or without
an optional asterisk), s
a1, a2, ..., an
.
Let be the unit vector
defined in spherical coordinates by
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(5)
|
Then the average value of the -component of the
over the surface
of the unit sphere is given by
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(6)
|
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(7)
|
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(8)
|
More generally,
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(9)
|
for ,
, or
(indexed as 1,
2, 3), and
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(10)
|
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(11)
|
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(12)
|
Given vectors ,
,
,
, the average values
of a number of quantities over the unit sphere are
given by
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(13)
|
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(14)
|
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(15)
|
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(16)
|
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(17)
|
and
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(18)
|
where is the Kronecker
delta,
is a dot
product, and Einstein summation has been
used.
A map that assigns each
a vector function
is called a
vector field.