Insights Slowly Lowering an Object in a Static, Spherically Symmetric Spacetime

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SUMMARY

This discussion focuses on the extraction of work when slowly lowering an object into a static, spherically symmetric gravitational field, utilizing the Einstein Field Equation and Maxwell’s Equations. The concept of potential energy is defined in this context, emphasizing the relationship between gravitational fields and energy extraction. The analysis builds on previous articles, providing a concrete understanding of potential energy through physical examples.

PREREQUISITES
  • Understanding of Einstein Field Equations
  • Familiarity with Maxwell’s Equations
  • Knowledge of gravitational fields and potential energy
  • Basic principles of classical mechanics
NEXT STEPS
  • Study the implications of the Einstein Field Equations in various gravitational contexts
  • Explore Maxwell’s Equations and their applications in electromagnetism
  • Research the concept of potential energy in different physical systems
  • Investigate the effects of radial motion on energy extraction in gravitational fields
USEFUL FOR

Physicists, students of general relativity, and anyone interested in the dynamics of gravitational fields and energy extraction methods.

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In the first two articles in this series, we looked at the Einstein Field Equation and Maxwell’s Equations in a static, spherically symmetric spacetime. Using formulas from those two previous articles, I now want to consider the question: what is the maximum amount of work that can be extracted by slowly lowering an object into a static, spherically symmetric gravitational field? This is a concrete, physical way of defining the concept of “potential energy”. (We’ll come back to the concept of “potential energy” and its relationship to other concepts of energy at the end of this article.)
We start with some comments and definitions. By “slowly lowering” we mean that the radial motion of the object is at some very slow, constant speed so that we...

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Likes vanhees71 and Greg Bernhardt
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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