Timeline for Massless charged particles
Current License: CC BY-SA 3.0
9 events
| when toggle format | what | by | license | comment | |
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| Nov 16, 2016 at 13:58 | comment | added | Luke Burns | Newton's law should be $F = dp/dt$ here, not $F = ma$. | |
| Feb 13, 2014 at 13:03 | history | edited | Hunter | CC BY-SA 3.0 |
Put the formulas into LaTeX
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| Feb 13, 2014 at 12:50 | review | Late answers | |||
| Feb 13, 2014 at 13:03 | |||||
| Feb 12, 2014 at 17:46 | comment | added | user34793 | Let us consider the particle's mass to be a function of (theta), In which case F_i = m(theta) a_i = 0 when (theta) = 90,where m(theta) = (rest mass) cos(theta),from this we realize that when theta = 0 ,I.e when it apears to be moving in space we realise F_i = F_j but F_i = (rest mass) a_i which contradicts the special relativIty since its speed would be c,therefore its rest would have to be infinite and when it is whizzing of at speeds greater than c we realize it would have complex.. | |
| Feb 12, 2014 at 13:12 | comment | added | Eelvex |
Since 'zero speed' is not invariant, any massless particle must move at c.
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| Feb 12, 2014 at 12:48 | history | edited | user34793 | CC BY-SA 3.0 |
changed the values for k
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| Feb 12, 2014 at 10:30 | history | edited | user34793 | CC BY-SA 3.0 |
added a few notes
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| S Feb 12, 2014 at 10:24 | history | answered | user34793 | CC BY-SA 3.0 | |
| S Feb 12, 2014 at 10:24 | history | made wiki | Post Made Community Wiki by user34793 |