I am a bit confused on how we can just say that (z',p) form a 4-vector. In my head, four vectors are sacred objects that are Lorentz covariant, but now we introduced some new variable and say it forms a 4-vector with momentum. I understand that these are just integration variables but I still do...
Where was the first term shown to be 0 / why would it be 0, this seems incorrect...?
I get your second reply specifying the off-shell condition but I do not see where you showed that ##\frac{\partial L}{\partial \phi} \delta \phi= 0##
Yes I understand both your points. I am just looking for a good detailed exposition of special relativity that is at the advanced undergraduate/ graduate level.
I am trying to learn special relativity well and I am finding it difficult to have good resources. So any concrete suggestions or recommendations would be helpful other than just "experience"!
Thanks for the enlightening answer. I do want to know however, why does the short cut work?
Moreover, you seem to have a great handle on the subject and I would like to gain the insight you have, what book on special relativity do you recommend? The chapters in Morin's and Taylor's classical...
Can you explain more? It would differ by the ##x' v/c^2## How does that "not make any difference" ?
Also does this mean it is true that they consider ##x' = 0## to obtain their result?
Would appreciate a more verbose, fully-fledged answer!
From the Lorentz transformation equations we know that $$t = \gamma(t^{'} - x^{'} v/c^2)$$
but for the Muon decay example where the setup is as follows :
"Assume for simplicity that a certain muon is created at a height of 50 km, moves straight downward, has a speed v = .99998 c, decays in...
Thank you Tazerfish for the excellent question. I also have the same question and am a bit disappointed at the answers.
This is an out of touch answer and also a bit rude. Look at any book textbook used in undergraduate/graduate physics : David Morin's classical mechanics, Griffith's E&M...
My issue is in deriving the coordinates of a point on a wheel that rotates without slipping. In Morin's solution he says that:
My attempt at rederiving his equation:
I do not understand how the triangle on the bottom with sides indicated in green is the same as the triangle on top that is...