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lecture_19
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| lecture_19 [2016/04/12 09:42] – rupert | lecture_19 [2017/05/06 10:14] (current) – rupert | ||
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| + | ===== The orthogonal projection of one vector onto another ===== | ||
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| + | Let $\def\ww{\vec{w}}\def\vv{\vec{v}}\def\uu{\vec{u}}\ww$ be a non-zero vector, and let $\vv$ be any vector. We call a vector $\def\pp{\vec p}\def\nn{\vec{n}}\pp$ the **orthogonal projection of $\vv$ onto $\ww$**, and write $\pp=\def\ppp{\text{proj}_{\ww}\vv}\ppp$, | ||
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| + | - $\pp$ is in the same direction as $\ww$; and | ||
| + | - the vector $\nn=\vv-\pp$ joining the end of $\pp$ to the end of $\vv$ is orthogonal to $\ww$. | ||
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| + | {{ : | ||
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| + | We can use these properties of $\pp$ to find a formula for $\pp$ in terms of $\vv$ and $\ww$. | ||
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| + | - Since $\pp$ is in the same direction as $\ww$, we have $\pp=c\ww$ for some scalar $c\in \mathbb{R}$. | ||
| + | - Since $\nn=\vv-\pp$ is orthogonal to $\ww$, we have $\nn\cdot \ww=0$. Hence \begin{align*}&& | ||
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| + | {{anchor: | ||
| + | \[ \pp=\ppp=\frac{\vv\cdot\ww}{\|\ww\|^2}\ww.\] | ||
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| + | We call $\nn=\vv-\ppp$ the component of $\vv$ orthogonal to $\ww$. | ||
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| === Example === | === Example === | ||
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| - Observe that $\uu\cdot (\vv\times \ww)=\vm{u_1& | - Observe that $\uu\cdot (\vv\times \ww)=\vm{u_1& | ||
| - | ==== Theorem ==== | + | ==== Theorem: the dot product/ |
| For any vectors $\vv$ and $\ww$ in $\mathbb{R}^3$, | For any vectors $\vv$ and $\ww$ in $\mathbb{R}^3$, | ||
| \[ \|\vv\times\ww\|^2+(\vv\cdot\ww)^2=\|\vv\|^2\, | \[ \|\vv\times\ww\|^2+(\vv\cdot\ww)^2=\|\vv\|^2\, | ||
| - | The proof is a tedious but elementary calculation, which we leave as an exercise. | + | === Proof === |
| + | Let $D$ be the sum of $v_i^2w_j^2$ over all $i, | ||
| + | |||
| + | Let $F$ be the sum of $v_i^2w_j^2$ over all $i, | ||
| + | |||
| + | Let $C$ be the sum of $v_iw_iv_jw_j$ over all $i, | ||
| + | |||
| + | Then $D+F$ is the sum of $v_i^2w_j^2$ over all $i,j\in \{1, | ||
| + | |||
| + | Expanding the formulae for $\|\vv\|^2$ and $\|\ww\|^2$, we get $\|\vv\|^2\|\ww\|^2=D+F$. | ||
| + | |||
| + | Expanding the formula for the cross product, we get $\|\vv\times\ww\|^2=F-2C$. | ||
| + | |||
| + | Expanding the formula for the dot product, we get $(v\cdot w)^2=D+2C$. | ||
| + | |||
| + | So $\|\vv\times\ww\|^2+(v\cdot w)^2=F-2C+D+2C=F+D=\|\vv\|^2\|\ww\|^2.■$ | ||
| ==== Corollary: the length of $\vec v\times\vec w$ ==== | ==== Corollary: the length of $\vec v\times\vec w$ ==== | ||
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| For any vectors $\vv$ and $\ww$ in $\mathbb{R}^3$, | For any vectors $\vv$ and $\ww$ in $\mathbb{R}^3$, | ||
| \[ \|\vv\times\ww\|=\|\vv\|\, | \[ \|\vv\times\ww\|=\|\vv\|\, | ||
| - | where $\theta$ is the angle between $\vv$ and $\ww$ (with $0\le\theta<\pi$). | + | where $\theta$ is the angle between $\vv$ and $\ww$ (with $0\le\theta\le\pi$). |
| === Proof === | === Proof === | ||
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| & | & | ||
| & | & | ||
| - | Since $\sqrt {a^2}=a$ if $a\ge0$ and $\sin\theta\ge0$ for $0\le\theta<\pi$, taking square roots of both sides gives | + | Since $\sqrt {a^2}=a$ if $a\ge0$ and $\sin\theta\ge0$ for $0\le\theta\le\pi$, taking square roots of both sides gives |
| \[ \|\vv\times\ww\|=\|\vv\|\, | \[ \|\vv\times\ww\|=\|\vv\|\, | ||
lecture_19.1460454124.txt.gz · Last modified: by rupert
