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any observer can make measurements and the precise numerical quantities obtained only depend on the coordinate system used.
any observer can make measurements and the precise numerical quantities obtained only depend on the coordinate system used.

* born coordinates, for another important coordinate system adapted to the motion of certain accelerated observers in minkowski spacetime.
* born coordinates, for another important coordinate system adapted to the motion of certain accelerated observers in minkowski spacetime.

the following example draws a line from (0, 0) to (200, 200) relative to the initial coordinate system.
(php 3 = 3.0.6, php 4)

for example, when measuring the electric and magnetic fields produced by an accelerating charge, the values of the fields will depend on the coordinate system used, but the fields are regarded as having an independent existence, this independence represented by the electromagnetic tensor.
for example, when measuring the electric and magnetic fields produced by an accelerating charge, the values of the fields will depend on the coordinate system used, but the fields are regarded as having an independent existence, this independence represented by the electromagnetic tensor .

this suggested a way of formulating relativity using 'invariant structures', those that are independent of the coordinate system (represented by the observer) used, yet still have an independent existence.
this suggested a way of formulating relativity using 'invariant structures', those that are independent of the coordinate system (represented by the observer) used, yet still have an independent existence.

for example, one strategy is to start with an ansatz (or an educated guess) of the final metric, and refine it until it is specific enough to support a coordinate system but still general enough to yield a set of simultaneous differential equations with unknowns that can be solved for.
for example, one strategy is to start with an ansatz (or an educated guess) of the final metric, and refine it until it is specific enough to support a coordinate system but still general enough to yield a set of simultaneous differential equations with unknowns that can be solved for.

10, 34–37, 1989*"the flagstaff measuring machine" (with d. monet), in iau symposium 141, inertial coordinate system on the sky, j.h.lieske and v.k.abalakin, eds., kluwer dordrecht 1990*"concluding remarks", in iau symposium 141, inertial coordinate system on the sky, j.h.lieske and v.k.abalakin, eds, kluwer dordrecht, 1990c. books or contributions to edited books*"the radio galaxy," sci.
10, 34–37, 1989*"the flagstaff measuring machine" (with d. monet), in iau symposium 141, inertial coordinate system on the sky, j.h.lieske and v.k.abalakin, eds., kluwer dordrecht 1990*"concluding remarks", in iau symposium 141, inertial coordinate system on the sky, j.h.lieske and v.k.abalakin, eds, kluwer dordrecht, 1990c. books or contributions to edited books*"the radio galaxy," sci.