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(I couldn't resist the title, because I am fed up with all the crackpot threads about why some aspect of modern physics is "incorrect".)
I work at an accelerator lab, dealing with particles whose velocities are not small compared with the speed of light. To me, saying that SR is incorrect is exactly like saying "the internal combustion engine is a fraud and does not work". It's a statement of such silliness as to leave one breathless. It is not as if I use some tiny piece of SR which is just small enough that I wiould get the same answer from another theory (which for example does not insist that simultaneity is relative). No, SR is fleshed out by me and others in excruciating mathematical detail, and if it is even a tiny bit wrong, our accelerator would not work!
Anyway, I thought I would share with everyone an aspect of the beauty of SR that I have never seen described anywhere else. Before SR, it was known that the pair of variables (t,E) acted very like the pairs (x,p_x), (y,p_y), (z,p_z). (These are called "canonical pairs".) It was known for example that in field-free regions,
[tex]E={p_x^2\over 2m}+{p_y^2\over 2m}+{p_z^2\over 2m}[/tex]
Hamilton showed that considering E to be a function of x,y,z,p_x,p_y,p_z, all the equations of motion could be derived from it. (It's called the "Hamiltonian".) For example, the equations could be derived from the "principal of least action", which involves the following integral
[tex]\int p_xdx+p_ydy+p_zdz-Edt[/tex]
Notice the symmetry (except for a sign change) between the afore-mentioned canonical pairs.
This symmetry obtains at a very deep level. For example, one could "pretend" that the independent variable is z instead of time t. Then all the equations would no longer answer the question, "Where is the particle at time t and what are its momentum components?", but rather, "I'm at z, so what are the x and y coordinates, the momenta p_x and p_y, and energy E and by the way, what time is it?" This can be obtained by solving the above E equation for p_z, and using p_z as if it were the new Hamiltonian. Amazingly, all the derived dynamics is exactly the same as if t were the independent variable.
There is truly a cyclic symmetry among x,y,z,t, and among p_x,p_y,p_z,E. All this was well-known before anyone ever dreamed of SR. So the question was: Why doesn't the equation for E display this symmetry explicitly? In fact the known dependence of E on momentum was very unsymmetric; for example, the momenta are squared, and the energy is not.
Then SR came along and everything made sense because:
[tex]E^2-p_x^2c^2-p_y^2c^2-p_z^2c^2=m^2c^4[/tex]
(or, in words, the norm of the 4-momentum is the rest energy). Notice the restoration of symmetry. Notice as well that this equation converges to the previous one (aside from a constant added to E) in the limit [itex]E<<mc^2[/itex]
Beauty, ain't it?
I work at an accelerator lab, dealing with particles whose velocities are not small compared with the speed of light. To me, saying that SR is incorrect is exactly like saying "the internal combustion engine is a fraud and does not work". It's a statement of such silliness as to leave one breathless. It is not as if I use some tiny piece of SR which is just small enough that I wiould get the same answer from another theory (which for example does not insist that simultaneity is relative). No, SR is fleshed out by me and others in excruciating mathematical detail, and if it is even a tiny bit wrong, our accelerator would not work!
Anyway, I thought I would share with everyone an aspect of the beauty of SR that I have never seen described anywhere else. Before SR, it was known that the pair of variables (t,E) acted very like the pairs (x,p_x), (y,p_y), (z,p_z). (These are called "canonical pairs".) It was known for example that in field-free regions,
[tex]E={p_x^2\over 2m}+{p_y^2\over 2m}+{p_z^2\over 2m}[/tex]
Hamilton showed that considering E to be a function of x,y,z,p_x,p_y,p_z, all the equations of motion could be derived from it. (It's called the "Hamiltonian".) For example, the equations could be derived from the "principal of least action", which involves the following integral
[tex]\int p_xdx+p_ydy+p_zdz-Edt[/tex]
Notice the symmetry (except for a sign change) between the afore-mentioned canonical pairs.
This symmetry obtains at a very deep level. For example, one could "pretend" that the independent variable is z instead of time t. Then all the equations would no longer answer the question, "Where is the particle at time t and what are its momentum components?", but rather, "I'm at z, so what are the x and y coordinates, the momenta p_x and p_y, and energy E and by the way, what time is it?" This can be obtained by solving the above E equation for p_z, and using p_z as if it were the new Hamiltonian. Amazingly, all the derived dynamics is exactly the same as if t were the independent variable.
There is truly a cyclic symmetry among x,y,z,t, and among p_x,p_y,p_z,E. All this was well-known before anyone ever dreamed of SR. So the question was: Why doesn't the equation for E display this symmetry explicitly? In fact the known dependence of E on momentum was very unsymmetric; for example, the momenta are squared, and the energy is not.
Then SR came along and everything made sense because:
[tex]E^2-p_x^2c^2-p_y^2c^2-p_z^2c^2=m^2c^4[/tex]
(or, in words, the norm of the 4-momentum is the rest energy). Notice the restoration of symmetry. Notice as well that this equation converges to the previous one (aside from a constant added to E) in the limit [itex]E<<mc^2[/itex]
Beauty, ain't it?