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Introducing LaTeX Math Typesetting

 
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Nov7-06, 07:43 AM   #766
 

Introducing LaTeX Math Typesetting


[tex]mc^2(\frac{hc}{\lambda_0}-\frac{hc}{\lambda_1})=\frac{hc}{\lambda_0}\frac{hc}{\lambda_1}(1-cos\theta)[/tex]
[tex]hmc^3(\frac{1}{\lambda_0}-\frac{1}{\lambda_1})=\frac{h^2c^2}{\lambda_0\lambda_1}(1-cos\theta)[/tex]
[tex]\lambda_0\lambda_1(\frac{1}{\lambda_0}-\frac{1}{\lambda_1})=\frac{h^2c^2}{hmc^3}(1-cos\theta)[/tex]
[tex]\lambda_1-\lambda_0=\frac{h}{mc}(1-cos\theta)[/tex]

[tex]E_0=hf_0[/tex] [tex]f_0=\frac{c}{\lambda_0}[/tex]
[tex]E_1=hf_1[/tex] [tex]f_1=\frac{c}{\lambda_1}[/tex]
 
Nov8-06, 09:31 PM   #767
 
Quote by HalfManHalfAmazing
[tex]\oint E\cdot dA = \frac{Q_{enc}}{\epsilon_0}[/tex]

Yahoo! Finally produced Gauss' Law in latex!
This would be better :

[latex]\oint_\mathcal{S} \mathbf{E} \cdot d\mathbf{A} = \frac{Q_\textrm{enc}}{\epsilon_0}[/latex]
 
Nov10-06, 12:58 AM   #768
 
Hi all,

Here is my question:

In the [tex]E>U_0[/tex] potential barrier, there should be no reflected wave when the incident wave is at one of the transmisson resonances. Assuming that a beam of particles is incident at the first transmission resonance, [tex]E=U_0+(\frac{\pi^2 h^2}{2mL^2})[/tex], combine the continuity conditions to show that B=0. Here are the continuity conditions:

1st [tex]A+B=C+D[/tex]

2nd [tex]k(A- B)=k^{'}(C-D)[/tex]

3rd [tex]Ce^{ik^{'}L}+De^{-ik^{'}L}=Fe^{ikL}[/tex]

4th [tex]k^{'}(Ce^{ik^{'}L}-De^{-ik^{'}L})=kFe^{ikL}[/tex]

A couple more equations that we already know are [tex]k=\sqrt{\frac{2mE}{h^2}}[/tex] and [tex]k^'=\sqrt{\frac{2m(E-U_0)}{h^2}[/tex]

Here is my attempted solution:

I divided the 4th equation by K and then set equation 3 and 4 equal to each other. I then used the new equation to solve for C in terms of D giving me

[tex]C=De^{-2i \pi}\frac{k^{'}+k}{k^{'}-K}[/tex] where I substituted [tex]\frac{\pi}{L}[/tex] in for k'.

I substituted this result into the first equation to now give me

[tex]A+B={De^{-2i \pi}\frac{k^{'}+k}{k^{'}-K} + D[/tex].

Solving for D gives me

[tex]\frac{A+B}{e^{-2i \pi}\frac{k^{'}+k}{k^{'}-K} + 1} = D[/tex]

Now, plugging in our solutions for D and C into the 2nd equation

[tex]\frac{(A+B)e^{-2i \pi}\frac{k^{'}+k}{k^{'}-K}}{e^{-2i \pi}\frac{k^{'}+k}{k^{'}-K}+1}-\frac{A+B}{e^{-2i \pi}\frac{k^{'}+k}{k^{'}-K}+1}=\frac{k}{k^{'}}(A-B})[/tex]

At this point, it seems impossible to simplify the equation to a point where it is obvious that B = 0. Am I on the right track or is there an easier way?
 
Nov12-06, 11:48 AM   #769
 
[tex]17(1-\frac{1}{17^2})^\frac{1}{2}[/tex]

Does anyone know of a website that allows me to use tex code and generate latex graphics, that isn't necessarily part of a forum like this one?

BTW, the guy who coded LaTeX into this forum is a bloody wizard.

EDIT: God! LaTeX is amazing! I've been checking the examples in this thread... what an invention!
 
Nov15-06, 06:04 AM   #770
 
Found one here: http://at.org/~cola/tex2img/index.php

(sorry for double post, I can't find the EDIT button...)
 
Nov15-06, 11:18 AM   #771
 
[tex]\frac{x-vt}{\sqrt{1-\frac{v^2}{c^2}}}[/tex]
[tex]\frac{x-vt}{\sqrt{2}}[/tex]
[tex]\sqrt{2}[/tex]
 
Nov15-06, 11:55 AM   #772
 
Admin
Blog Entries: 5
For testing please use:
http://at.org/~cola/tex2img/index.php
 
Jan21-07, 11:49 PM   #773
 
Admin
Blog Entries: 5
Here is another latex preview tool suggested by Ranger

http://rogercortesi.com/eqn/index.php
 
Jan25-08, 01:17 PM   #774
 
Mentor
Blog Entries: 1
FYI: Latex Command Window now available!
 
Jun30-08, 05:43 PM   #775
 
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Test...

[latex]A = A'[/latex]

- Warren
 
Oct22-08, 12:22 AM   #776
 
Recognitions:
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Test

[latex]E = mc^{10}[/latex]

???
 
Sep21-10, 05:54 PM   #777
 
Admin
Blog Entries: 5
This page can be used for unlimited LaTeX previewing and testing. It's a little crude. Still working some details out.

http://www.physicsforums.com/mathjax/test/preview.html
 
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