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lecture_18
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| lecture_18 [2015/04/02 10:55] – [Theorem: the relationship between angle and the dot product] rupert | lecture_18 [2017/04/06 10:04] (current) – rupert | ||
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| - | ==== Remark ==== | ||
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| - | $\|\vec{AB}\|$ is the distance from point $A$ to point $B$, since this is the length of vector which takes point $A$ to point $B$. | ||
| - | |||
| - | === Examples === | ||
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| - | * The distance from $A=(1,2)$ to $B=(-3,4)$ is $\|\def\m# | ||
| - | * 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, | ||
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| - | ==== Scalar multiplication and direction ==== | ||
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| - | Multiplying a vector by a scalar changes its length, but doesn' | ||
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| - | ==== Definition: unit vectors ==== | ||
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| - | {{page> | ||
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| - | ==== Proposition: | ||
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| - | 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 $\vec v$). | ||
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| - | === Proof === | ||
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| - | Using the formula $\|c\vec v\|=|c|\, | ||
| - | \[ \|\vec w\|=\left\|\frac1{\|\vec v\|}\vec v\right\|=\left|\frac1{\|\vec v\|}\right|\, | ||
| - | So $\vec w$ is a unit vector, and since it's scalar multiple of $\vec v$, it's in the same direction as $\vec v$. ■ | ||
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| - | ==== Example ==== | ||
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| - | What is unit vector in the same direction as $\vec v=\m{1\\2}$? | ||
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| - | We have $\|\vec v\|=\sqrt{1^2+2^2}=\sqrt5$, | ||
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| - | ===== Addition of vectors ===== | ||
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| - | If $\vec v=\vec{AB}$, | ||
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| - | If $\vec w=\vec {BC}$, then $\vec w$ moves $B$ to $C$, so $B+\vec w=C$. | ||
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| - | What about $\vec v+\vec w$? We have $A+\vec v+\vec w=B+\vec w=C$. So $\vec v+\vec w=\vec{AC}$. | ||
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| - | 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: | ||
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| - | {{ : | ||
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| - | 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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| - | {{ : | ||
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| ====== The dot product ====== | ====== The dot product ====== | ||
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| If $\vec v=\m{1\\2}$ and $\vec w=\m{-2\\1}$, | If $\vec v=\m{1\\2}$ and $\vec w=\m{-2\\1}$, | ||
| \[ 0=\dp vw=\sqrt 5\times \sqrt 5 \times \cos\theta\] | \[ 0=\dp vw=\sqrt 5\times \sqrt 5 \times \cos\theta\] | ||
| - | so $5\cos\theta=0$, | + | so $5\cos\theta=0$, |
| {{ : | {{ : | ||
| + | |||
| + | === Proof of the Theorem === | ||
| + | |||
| + | We wish to show that $\def\vv{\vec v} | ||
| + | \def\ww{\vec w}\vv\cdot\ww=\|\vv\|\, | ||
| + | |||
| + | Recall the [[wp> | ||
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| + | Consider a triangle with two sides $\vv$ and $\ww$. By the triangle rule for vector addition, the third side $\vec x$ has $\ww+\vec x=\vv$, so $\vec x=\vv-\ww$: | ||
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| + | Applying the cosine rule gives \[ \|\vv-\ww\|^2=\|\vv\|^2+\|\ww\|^2-2\|\vv\|\, | ||
| + | On the other hand, we know that $\|\vec x\|^2=\vec x\cdot\vec x$, so | ||
| + | \begin{align*}\|\vv-\ww\|^2& | ||
| + | So \[\|\vv\|^2+\|\ww\|^2-2\|\vv\|\, | ||
| + | |||
| + | ==== Corollary ==== | ||
| + | |||
| + | If $\vv$ and $\ww$ are non-zero vectors and $\theta$ is the angle between them, then $\cos\theta=\displaystyle\frac{\vv\cdot\ww}{\|\vv\|\, | ||
| + | |||
| + | ==== Corollary ==== | ||
| + | If $\vv$ and $\ww$ are non-zero vectors with $\vv\cdot\ww=0$, | ||
| + | |||
| + | ==== Examples ==== | ||
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| + | - The angle $\theta$ between $\def\c# | ||
| + | - The points $A=(2,3)$, $B=(3,6)$ and $C=(-4,5)$ are the vertices of a right-angled triangle. Indeed, we have $\vec{AB}=\c36-\c23=\c13$ and $\vec{AC}=\c{-4}5-\c23=\c{-6}2$, | ||
| + | - To find a unit vector orthogonal to the vector $\vv=\c12$, we can first observe that $\ww=\c{-2}1$ has $\vv\cdot\ww=0$, | ||
lecture_18.1427972110.txt.gz · Last modified: by rupert
