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This is a thread to practice latex, in case you have no idea what it is, please read our LaTeX tutorial.

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• 2 weeks later...

$E=mc^2$

About as far as I got.

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Testing...

$a^b$

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$\delta \Delta \frac{x}{\vec{x}}$$\huge a, b \cancel\delta$

god this is a bit nice...

$\cancel{a}$

$\delta aa \acute{50} ,\etc$

mmmm... so many others to try out!

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$f(x)=\int_{-\infty}^x\frac{(e^{-t^2})}{\sqrt{\pi^x}}dt$

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$\huge \int_{a}^{b}{e^{-14x}^{e}}{dx}$

Will this work?

$a^b^c^d^e^f^g^h$

staircase!

$\frac{X^5_G}{A_2}$

$\huge \frac{1}{\int^{\delta}_{{\delta}{\pi}} {x}^{\frac{987^{\frac{X^5_G}{\int^{a}_{e^{4123}}{x^{\frac{1.24}{L}}}{dx}}}}{\int_{low}^{high}{x^{x^{2e}}dx}}}dx}$

I guess some day or the other, this is going to give up on me. Lets see how much more complex I can make this, before it first shows signs of efficiency weakness.

Any human wanna solve this expression? No! don't run away!

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I guess it is my turn. Lessee...

$\Large f(t) = \int_{\small x=0}^{\small x=t}\frac{\sqrt{a x^3 + b x + c^2}}{e^{(c\pi x^2)}} dx\\ \normalsize\text{where a, b, c = integers >0}$

Cool beans!! Hot ****!! Ultimate power!!

Tomorrow... $\\ \huge\text{The World!}$

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Cool beans!! Hot ****!! Ultimate power!!

Tomorrow... $\\ \huge\text{The World!}$

Pinky and the Brain reference?

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.

Brain: There's only one ride that interests me - the incredible thrill ride of taking over the world!

Pinky: Mmm, I think there's a height requirement for that ride.

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[LATEX]test(1.\small{01}\normal)={\frac{1}{\infty^\pi} * 14x\sqrt{-1} = \huge{Sweet}[/LATEX]

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Well done, Pinky!! You have mathematically proven that no matter where you are on Earth, you are no more than 4 blocks away from the nearest Starbucks! Do you realized what this means?!?!?! It means I can...

$\huge\text{Take Over the World!!}$

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• 3 months later...

$\sim a_0 \sim 1\AA{\rm s}^{-2}$

Well that's udderly meaningless.

Found it here, per C1ay's news about the dark matter rebuttal.

http://arxiv.org/abs/astro-ph/0606216

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$\left( \sum_i \vec{\alpha}_i \cdot \vec{\nabla}_i + \sum_{i \neq j} \beta_{ij} \delta( \vec{x}_i - \vec{x}_j ) \right) \vec{\Psi} = K \frac{\partial}{\partial t} \vec{\Psi} = iKm \vec{\Psi}$

Courtesy of Doctordick. =)

http://home.jam.rr.com/dicksfiles/Explain/Explain.htm

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• 5 months later...

$\beta \gamma \ArrowBoldRightShort$

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• 2 months later... testing...

$\frac{d}{dx} © = 0$

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$\frac{d}{dx} (x) = 1$

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