Relativistic Frames of Reference: Difference between revisions

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From the Galilean description of motion for a frame of reference moving relative to another frame considered stationary we know that
From the Galilean description of motion for a frame of reference moving relative to another frame considered stationary we know that


<center><math>t \equal t'</math></center>
<center><math>t= t'</math></center>
 
<center><math>x=x'</math></center>
<center><math>x=x'</math></center>
<center><math>y=y'</math></center>
<center><math>y=y'</math></center>
<center><math>z=z'+vt</math></center>
<center><math>z=z'+vt</math></center>



Revision as of 02:56, 3 June 2017

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

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

Relativistic Frames of Reference

From the Galilean description of motion for a frame of reference moving relative to another frame considered stationary we know that

[math]\displaystyle{ t= t' }[/math]
[math]\displaystyle{ x=x' }[/math]
[math]\displaystyle{ y=y' }[/math]
[math]\displaystyle{ z=z'+vt }[/math]



Galilean Frames of Reference
Figure 2.1: Primed reference frame moving in the z direction with velocity v.




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

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