# LaTeX testing

## Recommended Posts

$A = \frac{(3.45 * 1200000)}{1,000,000} = 4.14$

Edited by Greg H.

##### Share on other sites

$r_s$

$r_s$

$$r_s$$

##### Share on other sites

${\small\begin{array}{|c|c|c|c|c|c|}\hline T_{Ho} (Gy) & T_{H\infty} (Gy) & S_{eq} & H_{0} & \Omega_\Lambda & \Omega_m\\ \hline 14.4&17.3&3400&67.9&0.693&0.307\\ \hline \end{array}}$ ${\small\begin{array}{|r|r|r|r|r|r|r|r|r|r|r|r|r|r|r|r|} \hline S&T (Gy)&R (Gly)&D_{now} (Gly)&D_{then}(Gly)&D_{hor}(Gly)&V_{gen}/c&H/Ho \\ \hline 1090.000&0.000373&0.000628&45.331596&0.041589&0.056714&21.023&22915.263\\ \hline 339.773&0.002496&0.003956&44.183524&0.130038&0.178562&10.712&3639.803\\ \hline 105.913&0.015309&0.023478&42.012463&0.396668&0.552333&5.791&613.344\\ \hline 33.015&0.090158&0.136321&38.051665&1.152552&1.651928&3.200&105.633\\ \hline 10.291&0.522342&0.785104&30.917756&3.004225&4.606237&1.782&18.342\\ \hline 3.208&2.977691&4.373615&18.247534&5.688090&10.827382&1.026&3.292\\ \hline 1.000&13.787206&14.399932&0.000000&0.000000&16.472274&1.000&1.000\\ \hline 0.312&32.884943&17.184900&11.117770&35.666086&17.224560&2.688&0.838\\ \hline 0.132&47.725063&17.291127&14.219438&107.785602&17.291127&6.313&0.833\\ \hline 0.056&62.598053&17.299307&15.535514&278.255976&17.299307&14.909&0.832\\ \hline 0.024&77.473722&17.299802&16.092610&681.060881&17.299802&35.227&0.832\\ \hline 0.010&92.349407&17.299900&16.328381&1632.838131&17.299900&83.237&0.832\\ \hline \end{array}}$

Oh my cosmocalc now works on this site

Edited by Mordred

##### Share on other sites
On 9/28/2017 at 11:19 AM, Strange said:

rs

rs

$$r_s$$

$$r_s$$

$r_s$

$r_s$

$\alpha={\cot}^{-1 }(\cos\upsilon\tan{\sin}^{-1}(\frac{\sin\frac{\lambda}{ 2}}{ \sin\upsilon}))$

Edited by steveupson

##### Share on other sites

$\rho \rightarrow \frac{\Lambda c^2}{8 \pi G}$

##### Share on other sites

Testing more latex

$\nabla ' (x,y,z,\omega_{s},\omega_{p},M,I,k,\phi,S,X,Z,\mu) = \sqrt{\hbar \omega_{s}(|Log_{(DgDa D \psi D \phi - W)}(\frac{2 \hbar G C^{2}R_{s} - \frac{1}{4}F^{a}_{\mu v}F^{a \mu v } + i(\psi bar)\gamma^{\mu}D_{\mu}\psi_{i} + (\psi bar)^{i}_{L}V_{ij}\phi \psi^{j}_{r} + a_{ij} - V(\phi)}{-D^{2}_{\mu}}|)(-e^{\frac{2S(r,t)}{h}}) - \frac {E_{Rest}}{C^{2}} \omega_{s} \sqrt{\frac{G_{uv} - R_{uv}}{-g_{uv}}} + {\frac{\frac{S R^{2}_{s}}{\Omega_{p}}}{2}}{\hbar^{2 \frac{2E_{rest}}{C^{2}}}}}$

Where both of the above are jacked up, I will fix the latex another time, those fractions..... are displaying wrong.

Edited by Vmedvil

##### Share on other sites




$\array{ \mathfrak{g} \times X && \overset{R}{\longrightarrow} && T X \\ & {\llap{pr_2}}\searrow && \swarrow_{\rlap{p}} \\ && X }$

$\array{e^+ \searrow &&\nearrow P^-\\&\leadsto &\\ e^-\nearrow &&\searrow P^+}$

$\tanh$

$pc$

$\wedge^\bullet_{C^\infty(X)} (\mathfrak{g}^\ast \otimes C^\infty(X)) \;=\; \underset{ deg = 0 }{ \underbrace{ C^\infty(X) }} \oplus \underset{ deg = 1 }{ \underbrace{ C^\infty(X) \otimes \mathfrak{g}^\ast }} \oplus \underset{ def = 2 }{ \underbrace{ C^\infty(X) \otimes \mathfrak{g}^\ast \wedge \mathfrak{g}^\ast }} \oplus \cdots$

$\array{ J^\infty_\Sigma(E)/T\Sigma \\ \downarrow \\ \Sigma/T\Sigma }$

Edited by Mordred

##### Share on other sites

$\boxed{\frac{ds}{dt} = 1 \cdot 10^{2} \; \frac{\text{m}}{\text{s}}} \; \; \; (100 \; \frac{\text{m}}{\text{s}})$