Dot Product of Vector with Itself
Jump to navigation
Jump to search
Theorem
Let $\mathbf u$ be a vector in the real vector space $\R^n$.
Then:
- $\mathbf u \cdot \mathbf u = \norm {\mathbf u}^2$
where $\norm {\mathbf u}$ is the length of $\mathbf u$.
Proof 1
Let $\mathbf u = \tuple {u_1, u_2, \ldots, u_n}$.
Then:
\(\ds \mathbf u \cdot \mathbf u\) | \(=\) | \(\ds u_1 u_1 + u_2 u_2 + \cdots + u_n u_n\) | Definition of Dot Product | |||||||||||
\(\ds \) | \(=\) | \(\ds u_1^2 + u_2^2 + \cdots + u_n^2\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \paren {\sqrt {\sum_{i \mathop = 1}^n u_i^2} }^2\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \norm {\mathbf u}^2\) | Definition of Vector Length in $\R^n$ |
$\blacksquare$
Proof 2
\(\ds \mathbf u \cdot \mathbf u\) | \(=\) | \(\ds \norm {\mathbf u} \norm {\mathbf u} \cos \angle \mathbf u, \mathbf u\) | Cosine Formula for Dot Product | |||||||||||
\(\ds \) | \(=\) | \(\ds \norm {\mathbf u}^2 \cos 0\) | since the angle between a vector and itself is $0$ | |||||||||||
\(\ds \) | \(=\) | \(\ds \norm {\mathbf u}^2\) | Cosine of Zero is One |
$\blacksquare$
Also presented as
This can also be seen presented as:
- $\norm {\mathbf u} = \paren {\mathbf u \cdot \mathbf u}^{1/2}$
or:
- $\norm {\mathbf u} = u = \sqrt {\mathbf u \cdot \mathbf u}$
and so on.
Sources
- 1927: C.E. Weatherburn: Differential Geometry of Three Dimensions: Volume $\text { I }$ ... (previous) ... (next): Introduction: Vector Notation and Formulae: Products of Vectors
- 1951: B. Hague: An Introduction to Vector Analysis (5th ed.) ... (previous) ... (next): Chapter $\text {II}$: The Products of Vectors: $2$. The Scalar Product: $(2.4)$
- 1992: Frederick W. Byron, Jr. and Robert W. Fuller: Mathematics of Classical and Quantum Physics ... (previous) ... (next): Volume One: Chapter $1$ Vectors in Classical Physics: $1.3$ The Scalar Product