Theta Dependent Components: Difference between revisions

From New IAC Wiki
Jump to navigation Jump to search
Vanwdani (talk | contribs)
No edit summary
Vanwdani (talk | contribs)
No edit summary
Line 9: Line 9:




 
=4.1.3.1  Theta Dependent Components=


<center>[[File:xz_lab.png | 400 px]]</center>
<center>[[File:xz_lab.png | 400 px]]</center>
Line 35: Line 35:


<center><math>\Longrightarrow p^'_{2(z)}\ should\ always\ be\ negative</math></center>
<center><math>\Longrightarrow p^'_{2(z)}\ should\ always\ be\ negative</math></center>
----





Revision as of 14:54, 30 May 2017

[math]\displaystyle{ \textbf{\underline{Navigation}} }[/math]

[math]\displaystyle{ \vartriangleleft }[/math] [math]\displaystyle{ \triangle }[/math] [math]\displaystyle{ \vartriangleright }[/math]


4.1.3.1 Theta Dependent Components

Figure 3: Definition of Moller electron variables in the CM Frame in the x-z plane.
Using [math]\displaystyle{ \theta '_2=\arccos \left(\frac{p^'_{2(z)}}{p^'_{2}}\right) }[/math]


[math]\displaystyle{ \Longrightarrow {p^'_{2(z)}=p^'_{2}\cos(\theta '_2)} }[/math]



Checking on the sign resulting from the cosine function, we are limited to:

[math]\displaystyle{ 90^\circ \le \theta '_2 \le 180^\circ \equiv \frac{\pi}{2} \le \theta '_2 \le \pi Radians }[/math]

Since,

[math]\displaystyle{ \frac{p^'_{2(z)}}{p^'_{2}}=cos(\theta '_2) }[/math]


[math]\displaystyle{ \Longrightarrow p^'_{2(z)}\ should\ always\ be\ negative }[/math]




[math]\displaystyle{ \textbf{\underline{Navigation}} }[/math]

[math]\displaystyle{ \vartriangleleft }[/math] [math]\displaystyle{ \triangle }[/math] [math]\displaystyle{ \vartriangleright }[/math]