The concept of a “Frame of Reference” gained relevance and prominence with the understanding of the implications of Einstein’s Theory of Special Relativity. Prior to that time, there was a consensus among physicists that there was a preferred frame of reference which was at “Absolute Rest.” In principal, all measurements taken could, in theory, be related to the frame at rest. They knew that the surface of the Earth was rotating once per day, and the Earth, itself, was orbiting the Sun, and the Sun was moving around the Galaxy, and so forth. But all these motions could be mathematically reduced by considering Absolute Rest as the frame of reference.
Or so they thought.
All that came crashing to the ground in 1887 with the spectacular failure of the Michelson–Morley experiment.
Their experiment was designed to measure the Earth’s motion with respect to the frame of absolute rest, and had the necessary precision to accomplish this. The continued failure, after many attempts, and by other researchers, to measure any motion was a thorn in the collective side of classical physicists of the day.
Einstein’s contribution to the resolution of this puzzle was to collect theoretical concepts which had been developed to explain the negative result, and draw them out to their full conclusion. Several researchers had given rigorous mathematical treatment to the transformations under which Maxwell’s equations were invariant. Many physicists, including George FitzGerald, Joseph Larmor, Hendrik Lorentz and Woldemar Voigt, had been discussing the physics behind these equations since 1887.
In particular, Einstein was able to derive the Lorentz Transformation equations from his Theory of Special Relativity.
This involves a term usually labeled [SIZE=2]γ ( the lower-case Greek letter “Gamma”.)[/SIZE]
1
γ = ______
[SIZE=2] √1-*v[sup]2[/sup]/c[sup]2[/sup]*
[/SIZE]
(read “gamma equals 1 divided by the square root of the quantity 1 minus velocity squared divided by c (speed of light) squared.”)
This term is essentially one (1) for velocities up to about 10% the speed of light in a vacuum.
It turns out that using this mathematical treatment resolves many discrepancies in the real world, and its value and significance has been tested and confirmed in many experiments.
A shorthand thought experiment would be:
Imagine you are flying past my position in a ship going a significant fraction of c. As you pass, in your moving frame of reference (from my point of view) you measure the length of your ship, while I, at relative rest, measure your ship from my frame of reference.
I will have measured a length (L[sub]me[/sub]) of your ship that differs from the length you measure (L[sub]you[/sub]), by an amount given by
L[sub]me[/sub] = L[sub]you[/sub] / [SIZE=2]γ[/SIZE]
[SIZE=2]that is, if, for example, you were moving at half the speed of light (c/2), the length I measure would be 86.6% of the length you measure on board your ship.
[/SIZE]The question “How long is the ship really?” is not relevant in this context. We each, in our own frame of reference, measure a length which is the “real” length from our point of view. This, in a nutshell, is the answer to your question about [capital “O”] Objectivity. There may be some objective reality “out there,” but the best we can do, any of us, is to describe it from our own frame of reference.