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lecture_17
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| - | ===== A more efficient way to find $A^{-1}$ | + | ====== Chapter 3: Vectors and geometry ====== |
| - | Given an $n\times | + | Recall that a $2\times |
| - | \[ \def\m#1{\left[ | + | |
| - | \begin{array}{@{} c|c {}@} % it does autodetection | + | |
| - | #1 | + | |
| - | \end{array} | + | |
| - | \right]}\m{A&I_n}\] | + | |
| - | and use [[EROs]] | + | |
| - | * Either you get a row of the form $[0~0~\dots~0~|~*~*~\dots~*]$ which starts with $n$ zeros. You can then conclude | + | We think of a (column) vector like $\vec v=\m{4\\3}$ as an instruction to move $4$ units to the right and $3$ units up. This movement is called " |
| - | * Or you end up with a matrix of the form $\m{I_n&B}$ for some $n\times n$ matrix | + | |
| + | === Examples === | ||
| + | |||
| + | The vector $\vec v=\m{4\\3}$ moves: | ||
| + | |||
| + | * $(0,0)$ to $(4,3)$ | ||
| + | | ||
| + | | ||
| + | |||
| + | It is convenient to not be too fussy about the difference between a point like $(4,3)$ and the vector $\m{4\\3}$. If we agree to write points as column vectors, | ||
| + | |||
| + | For example, we could rewrite the examples above by saying | ||
| + | |||
| + | * $\m{0\\0}$ to $\m{0\\0}+\m{4\\3}=\m{4\\3}$ | ||
| + | * $\m{-2\\6}$ to $\m{-2\\6}+\m{4\\3}=\m{2\\9}$ | ||
| + | * $\m{x\\y}$ to $\m{x\\y}+\m{4\\3}=\m{x+4\\y+3}$. | ||
| + | |||
| + | More generally: | ||
| + | |||
| + | === Example === | ||
| + | |||
| + | Which vector moves the point $A=(-1,3)$ to $B=(5, | ||
| + | |||
| + | Answer: we need a vector | ||
| + | |||
| + | ==== Definition of $\vec{AB}$ ==== | ||
| + | |||
| + | If $A$ and $B$ are any points in $\mathbb{R}^n$, | ||
| + | \[ \vec{AB}=B-A\] | ||
| + | (where on the right hand side, we interpret the points as column vectors so we can subtract them to get a column vector). | ||
| + | |||
| + | Thus $\vec{AB}$ is the vector which moves the point $A$ to the point $B$. | ||
| + | |||
| + | === Example === | ||
| + | |||
| + | In $\mathbb{R}^3$, the points $A=(3, | ||
| + | |||
| + | ==== The uses of vectors ==== | ||
| + | |||
| + | Vectors are used in geometry and science to represent quantities with both a **magnitude** (size/ | ||
| + | |||
| + | * displacements (in geometry) | ||
| + | * velocities | ||
| + | * forces | ||
| + | |||
| + | Recall that a column vector moves points. Its magnitude, or length, is how far it moves points. | ||
| + | |||
| + | ==== Definition: the length of a vector ==== | ||
| + | |||
| + | If $\vec v=\m{v_1\\v_2\\\vdots\\v_n}$ is a column vector in $\mathbb{R}^n$, | ||
| + | \[ \|\vec v\|=\sqrt{v_1^2+v_2^2+\dots+v_n^2}.\] | ||
| ==== Examples ==== | ==== Examples ==== | ||
| - | * Consider | + | * $\left\|\m{4\\3}\right\|=\sqrt{4^2+3^2}=\sqrt{16+9}=\sqrt{25}=5$ |
| - | \def\go#1#2{\m{\mat{#1}&\mat{#2}}} | + | * $\left\|\m{1\\0\\-2\\3}\right\|=\sqrt{1^2+0^2+(-2)^2+3^2}=\sqrt{1+0+4+9}=\sqrt{14}$ |
| - | \def\ar#1{\\[6pt]\xrightarrow{#1}&} | + | |
| - | \ar{R2\to R2-2R1}\go{1&3\\0& | + | ==== Exercise ==== |
| - | \end{align*} Conclusion: | + | |
| - | * Consider | + | Prove that if $c\in \mathbb{R}$ is a scalar and $\vec v$ is a vector in $\mathbb{R}^n$, then |
| - | \ar{R2\to R2-2R1}\go{1&3\\0&1}{1&0\\-2&1} | + | \[ \|c\vec v\|=|c|\,\|\vec v\|.\] |
| - | \ar{R1\to R1-3R1}\go{1&0\\0&1}{7& | + | That is, multiplying a vector by a scalar $c$ scales its length by $|c|$, the absolute value of $c$. |
| - | \end{align*} Conclusion: | + | |
| - | * Consider $A=\left[\mat{3&1&0\\-2& | + | ==== Remark ==== |
| - | \ar{R1\to R1+R2} | + | |
| - | \go{1& | + | $\|\vec{AB}\|$ is the distance from point $A$ to point $B$, since this is the length of vector which takes point $A$ to point $B$. |
| - | \ar{R2\to R2+2R1,\ R3\to R3-5R1} | + | |
| - | \go{1& | + | === Examples === |
| - | \ar{R3\leftrightarrow R2} | + | |
| - | \go{1& | + | * The distance from $A=(1,2)$ to $B=(-3,4)$ is $\|\def\m#1{\begin{bmatrix}#1\end{bmatrix}}\vec{AB}\|=\left\|\m{-3\\4}-\m{1\\2}\right\|=\left\|\m{-4\\2}\right\|=\sqrt{(-4)^2+2^2}=\sqrt{20}=2\sqrt{5}$. |
| - | \ar{R2\to R2+2R3} | + | * The length of the main diagonal of the unit cube in $\mathbb{R}^3$ is the distance between $0=(0,0,0)$ and $A=(1,1,1)$, which is $\|\vec{0A}\|=\left\|\m{1\\1\\1}\right\|=\sqrt{1^2+1^2+1^2}=\sqrt3$. |
| - | \go{1& | + | |
| - | \ar{R1\to R1+3R2,\ R3\to R3-10R2} | + | ==== Scalar multiplication and direction ==== |
| - | \go{1& | + | |
| - | \ar{R2\to R2+R3} | + | Multiplying a vector by a scalar changes its length, but doesn' |
| - | \go{1& | + | |
| - | \ar{R2\to -R2,\ R3\to -R3} | + | ==== Definition: unit vectors ==== |
| - | \go{1& | + | |
| - | \end{align*} | + | {{page> |
| + | |||
| + | ==== Proposition: | ||
| + | |||
| + | If $\vec v$ is a non-zero vector, then $\vec w=\frac1{\|\vec v\|}\vec v$ is a unit vector (in the same direction as $\vec v$). | ||
| + | |||
| + | === Proof === | ||
| + | |||
| + | Using the formula $\|c\vec v\|=|c|\,\|\vec v\|$ and the fact that $\|\vec v\|>0$, we have | ||
| + | \[ \|\vec w\|=\left\|\frac1{\|\vec v\|}\vec v\right\|=\left|\frac1{\|\vec v\|}\right|\,\|\vec v\|=\frac1{\|\vec v\|}\,\|\vec v\| = 1.\] | ||
| + | So $\vec w$ is a unit vector, and since it's scalar multiple of $\vec v$, it's in the same direction as $\vec v$. ■ | ||
| + | |||
| + | ==== Example ==== | ||
| + | |||
| + | What is unit vector in the same direction as $\vec v=\m{1\\2}$? | ||
| + | |||
| + | We have $\|\vec v\|=\sqrt{1^2+2^2}=\sqrt5$, so the proposition tells us that is $\vec w=\frac1{\|\vec v\|}\vec v = \frac1{\sqrt 5}\vec v=\frac1{\sqrt5}\m{1\\2}=\m{1/\sqrt{5}\\2/\sqrt5}$ is a unit vector in the same direction as $\vec v$. | ||
| + | |||
| + | ===== Addition of vectors ===== | ||
| + | |||
| + | If $\vec v=\vec{AB}$, then $\vec v$ moves $A$ to $B$, so $A+\vec v=B$. | ||
| + | |||
| + | If $\vec w=\vec | ||
| + | |||
| + | What about $\vec v+\vec w$? We have $A+\vec v+\vec w=B+\vec w=C$. So $\vec v+\vec w=\vec{AC}$. | ||
| + | |||
| + | This gives us the **triangle law for vector addition**: $\vec v$, $\vec w$ and $\vec v+\vec w$ may be arranged to form a triangle: | ||
| + | |||
| + | {{ : | ||
| + | We get another triangle by starting at $A$ and translating first by $\vec w$ and then by $\vec v$; the other side of this triangle is $\vec w+\vec v$. | ||
| + | But we know that $\vec v+\vec w=\vec w+\vec v$! So we can put these two triangles together to get the **parallelogram law for vector addition**: | ||
| + | {{ : | ||
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