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Thursday, 05.09.2024
That is, it would appear that any mathematical description can answer all hypothetical questions correctly only if it has embedded within it (explicitly or implicitly) a description of causes and their operations. Because those are all their properties, they ought to tell us everything about how they can act and interact, but we still would not know about the existence or the strength of any gravitational attraction. I would then ask whether the equation can also Continuants (Substances) Which Endure Through Change? what particular objects or particles might do if put in new situations? If it cannot, then it clearly falls short of the tasks physicists set themselves, and it would be useless for planning in engineering. But since these structural patterns only have significance in conjunction with the field equations, and because this conjunction results in true dispositions, the theory is not incompatible with reality of dispositions. That is, matter can be regarded as infiuencing the dispositions of objects to move in straight or curved paths. But if we are not satisfied with a purely instrumentalist account of scientific theories, we can still ask what is it about the physical world that makes this theory a correct description? Why does Online Casino - Online Poker differential equation correctly predict the world? Perhaps because it describes correctly the time evolution of dispositions such Online Casino - Play Poker forces, potentials, or quantum wave functions, in which case it can be construed as a good description of these real dispositions. Perhaps, however, it cannot be simply interpreted in this way, yet still gives good predictions of what actually happens. For now general relativity describes how the mass-energy tensor causes spacetime curvature, and the curvature itself in turn describes how objects would move in spacetime if they were present. Geometrodynamics (assuming the theory can be worked demarcate in adequate detail) has a similar thick sandwich time-dependent interpretation, but is different from general relativity in that now physical objects are not in spacetime (as we have always imagined), but simply are regions of spacetime with certain patterns of curvature. But this means that implicit in the non-linear field equations are rules for determining how a given pattern of curvature would interact Descartes And Leibniz various circumstances, on the basis of its nature as a pattern.