summaryrefslogtreecommitdiffstats
path: root/physics/special-relativity.page
diff options
context:
space:
mode:
Diffstat (limited to 'physics/special-relativity.page')
-rw-r--r--physics/special-relativity.page17
1 files changed, 9 insertions, 8 deletions
diff --git a/physics/special-relativity.page b/physics/special-relativity.page
index 9d60e3c..22bc666 100644
--- a/physics/special-relativity.page
+++ b/physics/special-relativity.page
@@ -1,11 +1,11 @@
-Special Relativity
-===========================
+---
+toc: no
+title: Special Relativity
+...
-Warning: This is a rough work in progress!! Likely to be factual errors,
- poor grammar, etc.
+.. warning: This is a rough work in progress!! Likely to be factual errors, poor grammar, etc.
-References: Most of this content is based on a 2002 Caltech course taught by
- Kip Thorn [PH237]
+.. note: Most of this content is based on a 2002 Caltech course taught by Kip Thorn [PH237]
As opposed to general relativity, special relativity takes place in a *flat*
Minkowski space time: a 4-space with three spatial dimensions and one time
@@ -46,11 +46,12 @@ Note the negative sign in front of the time dimension. The are three types of
separations: **space-like** when $(\Delta s)^2 > 0$, **null-** or
**light-like** when $(\Delta s)^2 = 0$, and **time-like** when
$(\Delta s)^2 < 0$. When dealing with time-like separations, ignore the
-implication of an imaginary number. The difference in time $\Delta \Tau$
-is always real: ($\Delta \Tau)^2= -(\Delta s)^2$.
+implication of an imaginary number. The difference in time $\Delta \mathrm{T}$
+is always real: ($\Delta \mathrm{T})^2= -(\Delta s)^2$.
References
----------------
[PH237]: **Gravitational Waves** (aka ph237), a course taught by Kip Thorne at Caltech in 2002. See http://elmer.tapir.caltech.edu/ph237/ for notes and lecture videos.
+