- #1
epr2008
- 44
- 0
My biggest qualm with the special theory of relativity and, for that matter, the general theory of relativity is the fact that both assume a little bit too much. My first area of skepticism is that so many cling to these as much as they do to Newton's laws, but there has been no tangible proof of either theory. While it seems to be very brilliant, it has also been proven logically and mathematically that beginning with a false statement can inevitably yield any result, and obviously even more so when that result is desired. This brings me to the foundation of the theories, the defined space-time interval given by
[tex]d{S^2} = d{l^2} - {(cdt)^2}[/tex].
My first question: Is there any proof that this is actually representative of "distance" in space-time? The theory clearly states that space and time are intimately connected, but this seems somewhat ill-posed as the definition of the interval obviously removes their dependence. I really do not know if this is a well-posed counterexample, but consider a stationary object in space with movement represented by a space-time coordinate system and let its position be the origin. Then after, say, one second for simplicity, the object has not moved and so
[tex]\begin{array}{l}
0 = {l^2} - {(ct)^2}\\
l = ct\\
l = 3.00 \times {10^8}{\rm{meters}}
\end{array}[/tex]
Which seems nonsensical since I stated that the object was stationary.
Next, I'd like to point out another assumption. Let [tex]{l^2} = {x^2} + {y^2} + {z^2}[/tex] we have
[tex]d{S^2} = d{x^2} + d{y^2} + d{z^2} - {(cdt)^2}[/tex]
Which brings me to my second question: Is there any proof that we occupy a 3 dimensional or even finite dimensional space, and is there even such a thing as "dimension"? For the former, it has become natural in mathematics that we represent spatial orientation by coordinates and coordinate axes, but this is merely a projection of actual space into an abstraction which we define. We can even project further into 2 dimensions and one dimension for special motions, and, because of transformational properties, orientation is preserved. But this still only says that these abstractions are projections and not actual representations. As for the latter, I do not think that there is a fathomable answer.
[tex]d{S^2} = d{l^2} - {(cdt)^2}[/tex].
My first question: Is there any proof that this is actually representative of "distance" in space-time? The theory clearly states that space and time are intimately connected, but this seems somewhat ill-posed as the definition of the interval obviously removes their dependence. I really do not know if this is a well-posed counterexample, but consider a stationary object in space with movement represented by a space-time coordinate system and let its position be the origin. Then after, say, one second for simplicity, the object has not moved and so
[tex]\begin{array}{l}
0 = {l^2} - {(ct)^2}\\
l = ct\\
l = 3.00 \times {10^8}{\rm{meters}}
\end{array}[/tex]
Which seems nonsensical since I stated that the object was stationary.
Next, I'd like to point out another assumption. Let [tex]{l^2} = {x^2} + {y^2} + {z^2}[/tex] we have
[tex]d{S^2} = d{x^2} + d{y^2} + d{z^2} - {(cdt)^2}[/tex]
Which brings me to my second question: Is there any proof that we occupy a 3 dimensional or even finite dimensional space, and is there even such a thing as "dimension"? For the former, it has become natural in mathematics that we represent spatial orientation by coordinates and coordinate axes, but this is merely a projection of actual space into an abstraction which we define. We can even project further into 2 dimensions and one dimension for special motions, and, because of transformational properties, orientation is preserved. But this still only says that these abstractions are projections and not actual representations. As for the latter, I do not think that there is a fathomable answer.