B Coleman 2003 Eur. J. Phys. 24 493 doi:10.1088/0143-0807/24/4/501
A dual first-postulate basis for special relativity
FREE ARTICLEB Coleman
CORRIGENDUM
This is a Corrigendum for the article 2003 Eur. J. Phys. 24 301
On page 305, the text and equation following equation (14) should read as follows.
If Ω is negative, then at 
, -z is infinite. Higher-order equi-recessive cascades would reduce this singularity threshold to any desired lower proportion of whatever 
might be (as mentioned by Rindler [17]); i.e.,
Velocity addition singularity excludes any finite negative value for Ω. (15)
On page 308, the labels T4 and t4 in figure 6 should be interchanged.
On page 309, the second part of equation (33) should read
.
On page 309, equation (35) should read
![T_n=\frac{T_{n-1} + vL +\sqrt{vT_{n-1}(vT_{n-1} + 2L)+G^2}}{(1-v^2)}\\ +\small\boldsymbol{} \frac{(1-v\Omega)[v^{2}T_{n-1} + vL + \sqrt{vT_{n-1}(vT_{n-1} + 2L)+G^2}]^2/(1-v^2)} {\sqrt{[vT_{n-1}+L+v\sqrt{vT_{n-1}(vT_{n-1} + 2L)+G^2}]^2(1-v)^2+(1-v^2)(1-v\Omega)^2(1-v^2\Omega)(G^2-L^2)}}.](http://ej.iop.org/images/0143-0807/24/4/501/img4.gif)
.
On page 311, in equation (40), p in the central denominator expression should be q.
- Dates
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Issue 4 (23 July 2003)
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A dual first-postulate basis for special relativity
B Coleman 2003 Eur. J. Phys. 24 493
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An elementary first-postulate measurement of the cosmic limit speed
Brian Coleman 2004 Eur. J. Phys. 25 L31
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