Inertial reference frames

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A local inertial reference frame can be established in a gravitational field either by positioning a small frame close to the source of curvature of space-time or by using a large frame far from it. The discussion raises the question of whether there is a quantitative relationship in general relativity between the mass/size of the reference frame and its distance from the curvature source. It is noted that if the reference frame has mass, it contributes to curvature, complicating the separation of effects. While a definitive relationship is not readily available, it is suggested that ambitious calculations could yield insights. The conversation highlights the complexities of creating inertial frames in the context of general relativity.
kurious
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I can make a local inertial reference frame in a gravitational field by creating a frame that is small but close to the source of curvature of space-time.
Alternatively I can make a local inertial reference frame by creating a frame that is large but a long distance from the source of curvature of space-time.
If the reference frame has a mass, is there a quantitative relationship in general relativity between the mass/size of the frame and its distance from the source of curvature of space-time?
 
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If the reference frame has a mass, then it IS a source of curvature, and cannot be separated from that.
 
kurious said:
I can make a local inertial reference frame in a gravitational field by creating a frame that is small but close to the source of curvature of space-time.
Alternatively I can make a local inertial reference frame by creating a frame that is large but a long distance from the source of curvature of space-time.
If the reference frame has a mass, is there a quantitative relationship in general relativity between the mass/size of the frame and its distance from the source of curvature of space-time?

Not one that is readily available but if one is ambitious it can be calculated. I'm not that ambitious though. :-)

Pete
 
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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