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| Argir Pando Vasil Dobri Matea Karagorgovi... |
 Posted: Thu Dec 03, 2009 6:02 am |
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and if so x = x0 + v t + v0 t0 breaks down to [x = v t]_{by any
index}. you were saying Galileo's and Einstein's relativity? well come
again please but skip Newton's ill differential mechanics! after all
in the beginning x cannot be function that depends only on time (say x
= 1 + 2 t + 3 t t; the adders left are not even addable among them
self) so in the end you can claim x = x0 + v0 t + a t t / 2 = function
(x0, v0, a, t). if some magnitude becomes constant it doesn't prevent
the function to continue depending on its unique units. try plotting x
= v t in wolfram's matematica:
http://www.wolframalpha.com/input/?i=Plot[v+t%2C+{v%2C+-4%2C+%2B4}%2C+{t%2C+-4%2C+%2B4}]
lesson: no more shitty kinetics right? find your self another way of
doing physics... |
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| M Purcell... |
| Posted: Thu Dec 03, 2009 7:25 am |
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Guest
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On Dec 3, 8:02 am, Argir Pando Vasil Dobri Matea Karagorgovi
<nada... at (no spam) gmail.com> wrote:
[quote]and if so x = x0 + v t + v0 t0 breaks down to [x = v t]_{by any
index}. you were saying Galileo's and Einstein's relativity? well come
again please but skip Newton's ill differential mechanics! after all
in the beginning x cannot be function that depends only on time (say x
= 1 + 2 t + 3 t t; the adders left are not even addable among them
self) so in the end you can claim x = x0 + v0 t + a t t / 2 = function
(x0, v0, a, t). if some magnitude becomes constant it doesn't prevent
the function to continue depending on its unique units. try plotting x
= v t in wolfram's matematica:
http://www.wolframalpha.com/input/?i=Plot[v+t%2C+{v%2C+-4%2C+%2B4}%2C+{t%2C+-4%2C+%2B4}]
lesson: no more shitty kinetics right? find your self another way of
doing physics...
[/quote]
Reminds me of Donald Shead's curvilinear analaysis, I wonder what
happened to him, maybe he tried to test it. Uncle Al might know, he
was pretty close. |
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