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Scalar Functions and Vector-valued Functions 📂Vector Analysis

Scalar Functions and Vector-valued Functions

Definition

Let DD be a subset DRnD\subset \mathbb{R}^{n} of the nn-dimensional Euclidean space.

  1. Functions having DD as their domain are called function of several variables.
  2. f:DRf : D \to \mathbb{R} is called a scalar function.
  3. For a scalar function f1,,fm:DRf_{1} , \cdots , f_{m} : D \to \mathbb{R}, f:DRm\mathbf{f} : D \to \mathbb{R}^{m} defined as follows is called a vector-valued function. f(x1,,xn):=[f1(x1,,xn)fm(x1,,xn)] \mathbf{f} ( x_{1} , \cdots , x_{n} ) : = \begin{bmatrix} f_{1} ( x_{1} , \cdots , x_{n} ) \\ \vdots \\ f_{m} ( x_{1} , \cdots , x_{n} ) \end{bmatrix}

Explanation

Function of Several Variables

Terms to denote a function of several variables include function of several variables, multivariable function, multivariate function, etc.

The term function of several variables is mainly used in analysis, including calculus. Originally, whether it’s a scalar function or a vector-valued function, it’s just a function. The term is used only to easily distinguish their codomains. From the perspective of linear algebra, if a vector-valued function is m=1m=1, it can be said to become a scalar function, so there is essentially no conceptual difference.

Scalar Function

As an example of scalar functions, consider F(m,a):=ma F ( m , a ) := ma. Whether mm is mass or aa is acceleration, to a mathematician, it should appear as a 22-dimensional vector like (m,a)([0,)×R)R2(m , a) \in \left( [0,\infty) \times \mathbb{R} \right) \subset \mathbb{R}^2. mama is simply the product of the two real numbers mm and aa, and since maRma \in \mathbb{R}, it well satisfies the condition of a scalar function. Meanwhile, in vector calculus, it is also called a Scalar Field since there is a scalar value corresponding to every point in the given space.

Vector-valued Function

As an example of vector-valued functions, consider
q(m,v,a):=[mamv12mv2] \mathbf{q} ( m , v , a ) : = \begin{bmatrix} ma \\ mv \\ {{1} \over {2}} m v^2 \end{bmatrix} . To a physicist, the components might respectively be force, momentum, and kinetic energy, but simply considering it as a vector-valued function it’s nothing more than q:DR3\mathbf{q} : D \to \mathbb{R}^3. Meanwhile, in vector calculus, it is also called a Vector Field since there is a vector corresponding to every point in the given space.