LaTeX Introducing LaTeX Math Typesetting

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SUMMARY

The Physics Forums has integrated LaTeX mathematical typesetting into its platform, allowing users to create professional-grade mathematical expressions. Users can include LaTeX graphics in posts using the [tex] and [itex] tags for display and inline formats, respectively. A PDF guide detailing essential LaTeX commands and symbols is available, along with additional resources for the amsmath package. This feature enhances the forum's capability for mathematical discussions and presentations.

PREREQUISITES
  • Familiarity with LaTeX syntax and commands
  • Understanding of mathematical notation and typesetting
  • Basic knowledge of using forums and posting content online
  • Access to LaTeX resources and documentation
NEXT STEPS
  • Explore the PDF guide on LaTeX commands provided by Physics Forums
  • Learn about the amsmath package and its functionalities
  • Practice creating LaTeX graphics using the [tex] and [itex] tags
  • Investigate additional LaTeX resources for advanced typesetting techniques
USEFUL FOR

Mathematicians, educators, students, and anyone involved in scientific communication who seeks to enhance their ability to present mathematical content effectively on online platforms.

  • #451
a^x_n ...

Edit: You left spaces in your brackets.
 
Last edited by a moderator:
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  • #452
hey how come i can't get it to work ??
 
  • #453
extreme_machinations said:
hey how come i can't get it to work ??
See my edits of your posts.
 
  • #454
\int_{0}^{\frac{\pi}{2}} \log \cos \kappa d \kappa
 
  • #455
Just trying...

\int_{0}^{\frac{\pi}{2}} \log \cos \Omega \ d \Omega

f(x) = \sin x, \mbox{if} \ x \ \epsilon \ (0, \frac{\pi}{2})
 
Last edited:
  • #456
f(x) = \left {\begin{array}{cc}\sin x,&\mbox{if} \ x \epsilon \ [0, \frac{\pi}{2})\\ \cos x, & \mbox{if} \ x \epsilon \ [\frac{\pi}{2}, \pi)\end {array}\right
 
  • #457
F=GmM_e/r^2
 
  • #458
aaahhaa! now that more like it
hey thanks doc
 
  • #459
f(x)=sinx^2
 
  • #460
int_{0}^{1} sinlogx
 
  • #461
\int_{0}^{1} sin^2logcosx dx
 
  • #462
This is a test

<br /> \begin{array}{1|c|c|c|c|c|}<br /> \text{Fixed Point}&amp;\text{Jacobian}&amp;\text{Eigenvalues}&amp;\text{Eigenvectors}&amp;\text{type}\\<br /> \hline<br /> (0,0)&amp;<br /> \left(\begin{array}{cc}1.5 &amp; 0 \\ 0 &amp; 2 \end{array}\right)&amp;<br /> 2,1.5 &amp;<br /> \left(\begin{array}{ca}0 \\ 1 \end{array}\right)<br /> \left(\begin{array}{ca}1 \\ 0 \end{array}\right)&amp;<br /> \text{Source}\\<br /> \hline<br /> <br /> (0,2)&amp;<br /> \left(\begin{array}{cc}0.5 &amp; 0 \\ -1.5 &amp; -2 \end{array}\right)&amp;<br /> -2,0.5 &amp;<br /> \left(\begin{array}{ca}0 \\ 1 \end{array}\right)<br /> \left(\begin{array}{ca}0.86 \\ -0.51 \end{array}\right)&amp;<br /> \text{Saddle}\\<br /> \hline<br /> <br /> (1.5,0)&amp;<br /> \left(\begin{array}{cc}-1.5 &amp; -0.75 \\ 0 &amp; 0.88 \end{array}\right)&amp;<br /> -1.5,0.88 &amp;<br /> \left(\begin{array}{ca}1 \\ 0 \end{array}\right)<br /> \left(\begin{array}{ca}-0.3 \\ 0.95 \end{array}\right)&amp;<br /> \text{Saddle}\\<br /> \hline<br /> <br /> (4/5,7/5)&amp;<br /> \left(\begin{array}{cc}-0.8 &amp; -0.4 \\ -1.05 &amp; -1.4 \end{array}\right)&amp;<br /> -1.8,-0.38 &amp;<br /> \left(\begin{array}{ca}0.37 \\ 0.93 \end{array}\right)<br /> \left(\begin{array}{ca}0.69 \\ -0.72 \end{array}\right)&amp;<br /> \text{Sink}\\<br /> \hline<br /> <br /> \end{array}<br />

Slick!
 
  • #463
extreme_machinations said:
\int_{0}^{1} sin^2logcosx dx


Doesn't look good.This one does.

\int_{0}^{1} \sin^{2}x \ln\cos x \ dx


Daniel.
 
  • #464
please help, i cannot find the 'does not equal' latex equation
 
  • #466
a \neq b

this should work
 
  • #467
next question, can i download this for my computer, i have a paper due when i return to school, and it will be a vast help to be able to type the symbols.
 
  • #468
Do NOT pay attention to this! (Just the triangle problem)--Do Not pay attention to this!
 
  • #469
Do NOT pay attention to this! (Just the triangle problem)--Do Not pay attention to this!

A\left( t \right) = \frac{{\left\| {\left[ {\vec r_2 \left( t \right) - \vec r_1 \left( t \right)} \right] \times \left[ {\vec r_3 \left( t \right) - \vec r_2 \left( t \right)} \right]} \right\|}}{2}
-----------------
And the coordinate system based on parameter t by unit vectors:

\vec u\left( t \right) = \frac{{\vec r_1 \left( t \right) - \vec r_2 \left( t \right)}}{{\left\| {\vec r_1 \left( t \right) - \vec r_2 \left( t \right)} \right\|}} \\

\vec v\left( t \right) = \frac{{\left[ {\vec r_3 \left( t \right) - \vec r_1 \left( t \right)} \right]\left\| {\vec r_1 \left( t \right) - \vec r_2 \left( t \right)} \right\|^2 - \left[ {\vec r_1 \left( t \right) - \vec r_2 \left( t \right)} \right]\left\{ {\left[ {\vec r_1 \left( t \right) - \vec r_2 \left( t \right)} \right] \cdot \left[ {\vec r_1 \left( t \right) - \vec r_3 \left( t \right)} \right]} \right\}}}{{\left\| {\left[ {\vec r_3 \left( t \right) - \vec r_1 \left( t \right)} \right]\left\| {\vec r_1 \left( t \right) - \vec r_2 \left( t \right)} \right\|^2 - \left[ {\vec r_1 \left( t \right) - \vec r_2 \left( t \right)} \right]\left\{ {\left[ {\vec r_1 \left( t \right) - \vec r_2 \left( t \right)} \right] \cdot \left[ {\vec r_1 \left( t \right) - \vec r_3 \left( t \right)} \right]} \right\}} \right\|}} \\ <br /> \end{array}

Again----Do NOT pay attention to this!
 
Last edited:
  • #470
Hello everybody

Sorry if this has been discussed already, I couldn't find anything like it:
How can I create a statement like
<br /> \hat{\xi}(g_0) \longrightarrow \infty \ (g_0 \rightarrow g_0^*),<br />
but with the second limit written smaller and below the first arrow?

Thanks, Bruno
 
  • #471
\hat{\xi}\left(g_{0}\right)\substack{\displaystyle{\longrightarrow}\\g_{0}\rightarrow g_{0}^{*}} \infty

Daniel.
 
  • #472
Here's a little modification of dextercioby's suggestion.
\hat{\xi}\left(g_{0}\right) <br /> \underset{ g_{0}\rightarrow g_{0}^{*} <br /> }{<br /> \overrightarrow{\qquad\qquad} <br /> }\<br /> \infty
or
\hat{\xi}\left(g_{0}\right) <br /> \underset{ g_{0}\rightarrow g_{0}^{*} <br /> }{<br /> \overrightarrow{\qquad} <br /> }\<br /> \infty
 
  • #473
Thank you! That's exactly what I've looked for.
 
  • #474
B_z=B_0(1-aZ)
 
  • #475
B_r=B_0br_0
 
  • #476
\int_0^5 f(x) dx = \frac{125}{3}
where f(x) = x^2
 
Last edited:
  • #477
U can use "{}" or "\qquad" or simply "space \ space" to place a space between "f(x)" and "dx".

Daniel.
 
  • #478
\ln(ab) = \int_1^{a} \frac{1}{t} dt + \int_a^{ab} \frac{1}{t} dt
 
  • #479
s = 1/2(u+v)t
 
  • #480
s = u+v/2*t
 

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