Difference between revisions of "Relativistic Frames of Reference"

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

[math]\vartriangleleft [/math] [math]\triangle [/math] [math]\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]t= t'[/math]
[math]x=x'[/math]
[math]y=y'[/math]
[math]z=z'+vt[/math]



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




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

[math]\vartriangleleft [/math] [math]\triangle [/math] [math]\vartriangleright [/math]