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lecture_19
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| Both sides previous revisionPrevious revisionNext revision | Previous revision | ||
| lecture_19 [2017/04/11 09:55] – [Theorem] rupert | lecture_19 [2017/05/06 10:14] (current) – rupert | ||
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| - Since $\nn=\vv-\pp$ is orthogonal to $\ww$, we have $\nn\cdot \ww=0$. Hence \begin{align*}&& | - Since $\nn=\vv-\pp$ is orthogonal to $\ww$, we have $\nn\cdot \ww=0$. Hence \begin{align*}&& | ||
| - | So | + | {{anchor: |
| \[ \pp=\ppp=\frac{\vv\cdot\ww}{\|\ww\|^2}\ww.\] | \[ \pp=\ppp=\frac{\vv\cdot\ww}{\|\ww\|^2}\ww.\] | ||
| Line 80: | Line 80: | ||
| - 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\, | ||
| Line 106: | Line 106: | ||
| 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 === | ||
| Line 115: | Line 115: | ||
| & | & | ||
| & | & | ||
| - | 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_19.1491904526.txt.gz · Last modified: by rupert
