MadSci Network: Physics |
There are at least two kinds of observers in quantum physics. At speeds much less than the speed of light, there are no relativistic effects to consider and so the definition of an observer can be concerned merely with the location of the observer relative the the particle or event to be observed. In most instances, speeds less than one tenth the speed of light are considered to be non-relativistic. At relativistic speeds, generally those greater than one tenth the speed of light, an inertial observer is needed. In special relativity (applied at relativistic speeds), a mouse, bacterium, computer, or another particle could not be an inertial observer. Instead, what is usually described as an inertial observer is more like a huge information gathering system, or a coordinate system for spacetime. There are differences between special and general relativity, but those are not particularly relevant for this response. To be inertial, the observer, or coordinate system must satisfy the following properties; 1) The distance between any two points in the coordinate system must be time independent, the distance is not different for different times, 2) The clocks, assumed distributed throughout the coordinate system, are synchronized (the time reported is not dependent on the location of the clock) and run at the same rate throughout the coordinate system (the observer), and 3) The geometry of space at any constant t is Euclidean. The simplest way to think of a Euclidean space is that it is a space (a coordinate system) in which the geometry most people are familiar with is applicable. If you were a mathematician, you would probably take issue with that last sentence, claiming it to be an oversimplification, but it should work in this instance. "An observation made by [an] inertial observer in the act of assigning to any event the coordinates x, y, z of the location of its occurrence and the time read by the clock at (x,y,z) when the event occurred. It is not the time t on the wrist watch worn by a scientist located at the origin (0,0,0) of the coordinate system when the scientist first observed the event." This quote is from pages 4 and 5 of Bernard F. Schutz's A First Course in General Relativity, Cambridge University Press, 1985 - the principal source I used in preparing this response. Thanks for the question, I hope this response helps.
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