Up to this point in Calculus III we have studied
functions whose domain is $\mathbb{R}$ and codomain is $\mathbb{R}^n$ (Chapter 13), and
functions whose domain is $\mathbb{R}^n$ and codomain is $\mathbb{R}$ (Chapters 14 and 15).
The logical conclusion to this course is thus the study of functions whose domain is $\mathbb{R}^n$ and codomain is $\mathbb{R}^m$.
We'll spend almost all of our efforts on the case when $m = n$. In this case we will regard the input of the function as points in $\mathbb{R}^n$ and the output of the function as $n$-vectors in $\mathbb{V}^n$.
Let $D \subseteq \mathbb{R}^n$. A vector field on $\mathbb{R}^n$ is a function
$$
\mathbf{F} :\mathbb{R}^n \to \mathbb{V}^n :\mathbf{x} \mapsto \mathbf{F}(\mathbf{x}),
$$
where $\mathbf{x} \in \mathbb{R}^n$ is regarded as a point in $D$, despite being written in vector notation. We will usually regard the output vector $\mathbf{F}(\mathbf{x})$ as being "attached" at $\mathbf{x}$; that is, $\mathbf{F}(\mathbf{x})$ is translated so that its initial point is $\mathbf{x}$.
Suppose $D \subseteq \mathbb{R}^2$. Then a vector field $\mathbf{F}$ on $D$ can be decomposed as
$$
\mathbf{F}(x,y) = \left\langle P(x,y), Q(x,y) \right\rangle,
$$
where $P$ and $Q$ are real-valued functions on $D$.
Suppose $D \subseteq \mathbb{R}^3$. Then a vector field $\mathbf{F}$ on $D$ can be decomposed as
$$
\mathbf{F}(x,y,z) = \left\langle P(x,y,z), Q(x,y,z), R(x,y,z) \right\rangle,
$$
where $P$, $Q$, and $R$ are real-valued functions on $D$.
Consider the vector field on $\mathbb{R}^2$ defined by
$$
\mathbf{F}(x,y) = y\ \mathbf{i} + (x+y)\ \mathbf{j}.
$$
Plug in some points in the plane and plot the corresponding vectors to get an idea of how this vector field behaves.
$\mathbf{x}$ | $\mathbf{F}(\mathbf{x})$ | $\mathbf{x}$ | $\mathbf{F}(\mathbf{x})$ |
---|---|---|---|
$(0,0)$ | $\langle 0, 0 \rangle$ | $\left(-\tfrac{1}{2},\tfrac{1}{2}\right)$ | $\left\langle -\tfrac{1}{2}, 0 \right\rangle$ |
$(1,0)$ | $\langle 0,1 \rangle$ | $(-1,0)$ | $\langle 0,-1 \rangle$ |
$\left(\tfrac{1}{2},\tfrac{1}{2}\right)$ | $\left\langle \tfrac{1}{2}, 1 \right\rangle$ | $\left(-\tfrac{1}{2},-\tfrac{1}{2}\right)$ | $\left\langle -\tfrac{1}{2}, -1 \right\rangle$ |
$\left( 1,0 \right)$ | $\left\langle 1,1 \right\rangle$ |
$(0,-1)$ | $\langle -1, -1 \rangle$ |
Newton's Law of Gravitation states that the magnitude of the gravitational force between two objects whose masses are $m$ and $M$ (both positive constants) is given by
$$
\big\Vert\mathbf{F}(r)\big\Vert = \frac{mMG}{r^2},
$$
where $\mathbf{F}$ is the gravitational force field, $G$ is the gravitational constant, and $r$ is the distance between the centers of mass of the two objects.
Work out a formula for the gravitational field $\mathbf{F}$ exerted by an object of mass $M$ whose center of mass is the origin, on an object of mass $m$ whose center of mass is located at the point $(x,y,z)$ in $3$-dimensional space.
One of the most important classes of examples of a vector field is one that we have already begun to study.
Suppose $f$ is a differentiable function on a domain $D \subseteq \mathbb{R}^2$. The gradient vector field along $f$ (or corresponding to $f$) is the vector field on $D$ defined by
$$
\nabla f(x,y) = \left\langle \frac{\partial f}{\partial x}(x,y), \frac{\partial f}{\partial y} (x,y) \right\rangle,
$$
or more succinctly, $\nabla f = \langle \partial_x f,\partial_y f \rangle$.
If $f$ is a function defined on a domain in $\mathbb{R}^3$, its gradient vector field is defined analogously. It is given by
$$
\nabla f = \langle \partial_x f,\partial_y f,\partial_z f \rangle.
$$
The vectors of a gradient field are orthogonal to the level curves of the function $f$.
Plot the gradient field and a few level curves for the function
$$
f(x,y) = \tfrac{1}{2}\left( x^2 - y^2 \right).
$$
Suppose a particle is moving in a velocity field $\mathbf{V}$. At any point $(x,y,z)$ in the domain, the particle's velocity is given by
$$
\mathbf{V}(x,y,z) = \left\langle x^2, z + y^2, 2xyz \right\rangle.
$$
If a particle is dropped into the velocity field (with $\mathbf{0}$ acceleration) at the point $(3,2,1)$, estimate the particle's location after $0.1$ seconds.
Given the vector field
$$
\mathbf{F}(x,y) = \left\langle 3y\sin x + 3xy\cos x, 3x\sin x \right\rangle,
$$
is it possible to find a function $f$ such that $\mathbf{F} = \nabla f$? If not, why? If so, find one.
Questions? You can ask them here.
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