Causation and the Conservation of Energy in General Relativity.

Consensus in the contemporary philosophical literature has it that conserved quantity theories of causation such as that of Dowe—according to which causation is to be analysed in terms of the exchange of conserved quantities (for example, energy)—face damning problems when confronted with contempora...

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Publicado en:British Journal for the Philosophy of Science Vol. 77; no. 3; pp. 867 - 895
Autores principales: Ramírez, Sebastián Murgueitio, Read, James, Páez, Andrés
Formato: Artículo
Publicado: University of Chicago Press Sep2026
Materias:
Acceso en línea:Ver este registro en EBSCOhost
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        atl: Causation and the Conservation of Energy in General Relativity.
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        au:
          Ramírez, Sebastián Murgueitio
          Read, James
          Páez, Andrés
        affil:
          Philosophy Department. Princeton University. Princeton, NJ, USA.
          Faculty of Philosophy. University of Oxford. Oxford, UK.
          Department of Philosophy. Universidad de los Andes. Bogotá, Colombia.
      su:
        Conservation of energy
        General relativity (Physics)
        Causation (Philosophy)
        Calculus of tensors
        Philosophy of science
        Conserved quantity
        Scientific method
        Symmetries (Quantum mechanics)
      sug:
        subj:
          Conservation of energy
          General relativity (Physics)
          Causation (Philosophy)
          Calculus of tensors
          Philosophy of science
          Conserved quantity
          Scientific method
          Symmetries (Quantum mechanics)
      ab: Consensus in the contemporary philosophical literature has it that conserved quantity theories of causation such as that of Dowe—according to which causation is to be analysed in terms of the exchange of conserved quantities (for example, energy)—face damning problems when confronted with contemporary physics, where the notion of conservation becomes delicate. In particular, it is often claimed that in general relativity there simply are no conservation laws for (say) total stress-energy. If this claim is correct, it is difficult to see how conserved quantity theories of causation could survive. In this article, we resist the above consensus and defend conserved quantity theories from this conclusion, at least when focusing on the apparent problems posed by general relativity. We argue that this approach to causation can continue to be defended in general relativity, once one appreciates the availability of approximate symmetries in generic general relativistic spacetimes, and the role of modelling and idealization in that theory. Given these points, conserved quantity theories of causation must stand or fall on other grounds.
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    language: English
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