Vector Space
A vector space over a field $F$ is a set $V$ together with two operations: - Vector addition: $V \times V \to V$ - Scalar multiplication: $F \times V \to V$
satisfying the following axioms:
Referenced by (3 direct, 32 transitive)
Direct references:
Transitive (depth 1):
- remark-9
- remark-16
- Hessian Matrix
- incompressible
- Bound vector
- Direction
- invariance-of-curl
- Jacobian Matrix
- Cross Product
- Unit Vector
- note-5
- Surface Normal Vector
- theorem-19
- remark-45
- Free vector
- remark-32
- Vector Multiplication by a Scalar
- note-3
Transitive (depth 2):
- Vector Equality
- proof-of-theorem-19
- remark-46
- Normal Derivative
- Directional Derivative
- Zero Vector
- remark-30
- directional-derivative-is-inner-product-of-vector-and-grad
- remark-23
- Tangent Vector
- gradient-as-surface-normal-vector
- proof-of-gradient-as-surface-normal-vector
Transitive (depth 3):
Scalars
A scalar is an element of a field used to define a vector space.
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Typically, especially in physics, a scalar is simply a number, especially a real number.
Vectors
A vector is an element in a vector space.
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Direct references:
Transitive (depth 1):
- Vector Equality
- proof-of-theorem-19
- remark-46
- Normal Derivative
- Directional Derivative
- Zero Vector
- remark-30
- directional-derivative-is-inner-product-of-vector-and-grad
- remark-23
- Tangent Vector
- gradient-as-surface-normal-vector
- proof-of-gradient-as-surface-normal-vector
Transitive (depth 2):
Typically, in physics and many other applications, when we say vector we mean a vector in $\mathbb{R}^n,$ which is an ordered tuple of real numbers, $\vec{x} = (x_1, x_2, \cdots, x_n).$ This is the algebraic representation of vector $\vec{x}$.
The geometric representation of vector $\vec{x}$ is, in an $n$ dimensional space, an arrow or directed line segment. When starting from the origin, it would be a line segment from $\vec{0}$ to the point $(x_1, x_2, \cdots, x_n)$.
Physically, a vector has a magnitude and a direction.
A vector with a fixed endpoint is called a bound vector.
Properties of Vectors
Let $\vec{x} = (x_1, x_2, \cdots, x_n) \in \mathbb{R}^n$. The magnitude, or length, $\vec{x}$ is denoted as $|| \vec{x} ||$ and is defined as:
$$ ||\vec{x}|| = \sqrt{ {x_1}^2 + {x_2}^2 + \cdots + {x_n}^2 } = \sqrt{\vec{x} \cdot \vec{x}} = \sqrt{\sum_{i=1}^n x_i^2} $$
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This is essentially the Pythagorean theorem in $n$ dimensions; in $\mathbb{R}^2$ the magnitude of a vector corresponds to the length of the hypotenuse of a right triangle whose other sides are of length $x_1$ and $x_2.$
While we define norm to be equivalent to magnitude here, this is actually a special case of the more general concept of a norm - there are other norms we could define on $\mathbb{R}^n,$ but I don't have need to explore that yet.
The direction of a vector can be specified by the angle between it and some fixed reference, such as the $x$-axis.
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The zero vector $(0, 0, \cdots, 0)$ is denoted as $\vec{0}$ and has no direction.
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We perform vector addition by adding two vectors $\vec{x} = (x_1, x_2, \cdots, x_n)$ and $\vec{y} = (y_1, y_2, \cdots, y_n)$ according to the following rule:
$$ \vec{x} + \vec{y} = (x_1 + y_1, x_2 + y_2, \cdots, x_n + y_n) $$
that is, by making a new vector where the coordinates are the sums of the respective coordinates in the vectors being summed.
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Geometrically, vector addition connects vectors head to tail.
Similarly, vector subtraction can be performed as:
$$ \vec{x} - \vec{y} = (x_1 - y_1, x_2 - y_2, \cdots, x_n - y_n) $$
Multiplication
If $\vec{x}$ and $\vec{y}$ are vectors in $\mathbb{R}^n,$ then their inner product is defined as
$$ \vec{X} \cdot \vec{y} = \sum_{i = 1}^n x_i y_i. $$
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Transitive (depth 1):
The dot product of $\vec{u}$ and $\vec{v}$ is
$$ \vec{u} \cdot \vec{v} = |\vec{u}||\vec{v}|\cos{\theta} $$
where $\theta$ is the angle between $\vec{u}$ and $\vec{v}.$
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Two vectors $\vec{u}$ and $\vec{v}$ are said to be perpendicular or orthogonal if the angle between them is $\pi/2$ radians, or, equivalently, if the inner product $\vec{u} \cdot \vec{v} = 0.$
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Transitive (depth 1):
Transitive (depth 2):
Two vectors $\vec{x}$ and $\vec{y}$ are said to be parallel if $\vec{x}$ is a scalar multiple of $\vec{y}$, i.e., if there exists some scalar $c$ where $\vec{x} = c \vec{y}.$
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The cross product $\vec{a} \times \vec{b}$ (read "a cross b") of two vectors $\vec{a}$ and $\vec{b}$ is the vector $\vec{v}$ denoted by
$$ \vec{v} = \vec{a} \times \vec{b}. $$
I. If $\vec{a} = \vec{0}$ or $\vec{b} = \vec{0},$ then we define $\vec{v} = \vec{a} \times \vec{b} = \vec{0}.$
II. If both vectors are nonzero vectors, then vector $\vec{v}$ has the length
$$ \tag{1} |\vec{v}| = |\vec{a} \times \vec{b}| = |\vec{a}||\vec{b}|\sin{\theta}, $$
where $\theta$ is the angle between $\vec{a}$ and $\vec{b}.$ Furthermore, $\vec{a}$ and $\vec{b}$ form the sides of a parallelogram on a plane in space. The area of this parallelogram is precisely given by (1), such that the length $|\vec{v}|$ of the vector $\vec{v}$ is equal to the area of the parallelogram.
III. If $\vec{a}$ and $\vec{b}$ lie in the same straight line, i.e. $\vec{a}$ and $\vec{b}$ have the same or opposite directions, then $\theta$ is $0 \degree$ or $180 \degree$ so that $\sin \theta = 0.$ In that case $|\vec{v}| = 0,$ so that $\vec{v} = \vec{a} \times \vec{b} = \vec{0}. $$
IV. If cases I and III do not occur, then $\vec{v}$ is a nonzero vector. The direction of $\vec{v} = \vec{a} \times \vec{b}$ is perpendicular to both $\vec{a}$ and $\vec{b}$ such that $\vec{a}, \vec{b}, \vec{v},$ precisely in this order, form a right-handed triple
Referenced by (1 direct)
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If $\vec{a} = (a_1, a_2, a_3)$ and $\vec{b} = (b_1, b_2, b_3),$ then we use the symbolic determinant to find the cross product, in this fashion:
$$ \vec{v} = \vec{a} \times \vec{b} = \begin{vmatrix}\vec{i} & \vec{j} & \vec{k}\\a_1 & a_2 & a_3\\b_1 & b_2 & b_3\end{vmatrix} = \begin{vmatrix} a_2 & a_3 \\ b_2 & b_3 \end{vmatrix} \vec{i} - \begin{vmatrix} a_1 & a_3 \\ b_1 & b_3 \end{vmatrix} \vec{j} + \begin{vmatrix} a_1 & a_2 \\ b_1 & b_2 \end{vmatrix} \vec{k}. $$
Let $\vec{v_1}, \vec{v_2}, \cdots, \vec{v_n} \in \mathbb{R}^n$ and $c_1, c_2, \cdots, c_3 \in \mathbb{R}.$ Then, the vector
$$ \vec{v} = c_1 \vec{v_1} + c_2 \vec{v_2} + \cdots + c_n \vec{v_n} $$
is called a linear combination of $\vec{v_1}, \vec{v_2}, \cdots, \vec{v_n}.$
Let $\vec{v_1}, \vec{v_2}, \cdots, \vec{v_n} \in \mathbb{R}^n.$ The set of all linear combinations of $\vec{v_1}, \vec{v_2}, \cdots, \vec{v_n}$ is called their span, denoted $\Span{\left(\vec{v_1}, \vec{v_2}, \cdots, \vec{v_n}\right)}.$
That is:
$$ \Span{\left(\vec{v_1}, \vec{v_2}, \cdots, \vec{v_n}\right)} = \left\{ \vec{v} \in \mathbb{R}^n : \vec{v} = c_1 \vec{v_1} + c_2 \vec{v_2} + \cdots + c_n \vec{v_n} ~ \text{for some scalars} ~ c_1, c_2, \cdots, c_n \right\} $$