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John Denker has asked if I consider everyone who speaks of energy
density to be in error. Of course I do not; figures of speech and
conventional conveniences are useful. Energy density is a useful
concept. John, please tell me how you view the energy density in a
gravitational field.
There are many conservation laws in Nature. Is linear momentum a
substantial entity? Angular momentum? No, neither is real.
When a
gravitational system contains just two bodies we know the familiar
conserved quantities serve well. There are *ten* known scalar
quantities that are conserved in celestial mechanical systems.
Three are linear momentum components, three angular momentum
components, total energy, and three others called "integrals of
area". All are invariant, and none is substantial.
Why must energy be special?
Leigh
...*there are no blocks* -Feynman