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404 | 404 | \begin{theorem}{Solution and Orthogonality} |
405 | 405 | If $A$ is an $m \times n$ matrix, then the solution set of the homogeneous linear system $A\mathbf{x} = \mathbf{0}$ consists of all vectors in $\mathbb{R}^{n}$ that are orhtogonal to every row vector in $A$. |
406 | 406 | \end{theorem} |
| 407 | + \subsection{Equations Summary} |
| 408 | + \begin{sidenote}{Equations of a Plane} |
| 409 | + Let $\mathbf{n} = \left\langle a, b, c\right\rangle$ be a vector \emph{orthogonal} to the plane, and $\mathbf{r_{0}} = (x_{0}, y_{0}, z_{0})$ be a point on the plane. Let $\mathbf{v_{1}}$ and $\mathbf{v_{2}}$ be vectors parallel to the plane. |
| 410 | + \begin{center} |
| 411 | + \begin{tblr}{ll} |
| 412 | + Point Normal: & $a(x - x_{0}) + b(y - y_{0}) + c(z - z_{0}) = 0$\\ |
| 413 | + General Form: & $ax + by + cz + d = 0$\\ |
| 414 | + Vector Form: & $\mathbf{n} \cdot (\mathbf{r} - \mathbf{r_{0}})$ \nl |
| 415 | + $(a, b, c)(x - x_{0}, y - y_{0}, z - z_{0}) = 0$\\ |
| 416 | + Parametric Form: & $\mathbf{r} = \mathbf{r_{0}} + t_{1}\mathbf{v_{1}} + t_{2}\mathbf{v_{2}}$ |
| 417 | + \end{tblr} |
| 418 | + \end{center} |
| 419 | + \end{sidenote} |
| 420 | + \begin{sidenote}{Equations of a Line in $2$-space} |
| 421 | + Let $\mathbf{n} = \left\langle a, b, c\right\rangle$ be a vector \emph{parallel} to the line, and $\mathbf{r_{0}} = (x_{0}, y_{0}, z_{0})$ be a point on the line. |
| 422 | + \begin{center} |
| 423 | + \begin{tblr}{ll} |
| 424 | + Point Normal: & $a(x - x_{0}) + b(y - y_{0}) = 0$\\ |
| 425 | + General Form: & $ax + by + c = 0$\\ |
| 426 | + Vector Form: & $\mathbf{n} \cdot (\mathbf{r} - \mathbf{r_{0}}) = 0$ \nl |
| 427 | + $(a, b)(x - x_{0}, y - y_{0}) = 0$\\ |
| 428 | + Parametric Form: & $\mathbf{r} = \mathbf{r_{0}} + t\mathbf{n}$ \nl |
| 429 | + $ (x, y) = (x_{0}, y_{0}) + t(a, b)$\\ |
| 430 | + Parametric Equations: & $x = x_{0} + at$ \nl |
| 431 | + $y = y_{0} + bt$ |
| 432 | + \end{tblr} |
| 433 | + \end{center} |
| 434 | + \end{sidenote} |
| 435 | + \subsection{Symmetric Equations} |
| 436 | + \begin{definition}{Symmetric Equation} |
| 437 | + The \concept{symmetric equations} of a line $L$ in $3$-space are given by: |
| 438 | + \begin{align*} |
| 439 | + \frac{x - x_{0}}{a} = \frac{y - y_{0}}{b} = \frac{z - z_{0}}{c} |
| 440 | + \end{align*} |
| 441 | + where $(x_{0}, y_{0}, z_{0})$ is a point passing through the line, and $\mathbf{v} = \left\langle a, b, c\right\rangle $ is a vector parallel to the line. This vector is called the \concept{direction vector}. |
| 442 | + \end{definition} |
407 | 443 | \rulechapterend |
408 | 444 | \end{document} |
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