Inhomogeneous Wave Eq. & Minkowski Spacetime Interval

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Prez Cannady
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Answer is probably not, but is there some connection between the inhomogeneous wave equation with a constant term and the spacetime interval in Minkowski space?

$$
1) ~~ \nabla^2 u - \frac{1}{c^2} \frac{\partial^2 u}{\partial t^2} = \sum_{i=0}^2 \frac{\partial^2 u}{\partial x_i^2} - \frac{1}{c^2} \frac{\partial^2 u}{\partial t^2} = S
$$
$$
2) ~~ \sum_{i=0}^2 dx_i^2 - c^2 dt^2 = ds^2
$$
 
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on Phys.org
The only connection I can think of, is that you use the very same metric in both equations. But I suspect you're looking for connections which aren't to be found.
 
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Tensorially, these are written as
[itex]g^{ab}\nabla_a\nabla_b u=S[/itex]
[itex]g_{ab}ds^a ds^b=ds^2[/itex]

Using the shorthand
[itex]\nabla^b\equiv g^{ab} \nabla_a[/itex]
[itex]ds_{b}\equiv g_{ab}ds^a[/itex]
known as raising and lowering indices,
we have
[itex]\nabla^b\nabla_b u=S[/itex]
[itex]ds_b ds^b=ds^2[/itex]

Using more index-gymnastics,
we can write
[itex]\nabla^b\nabla_b u=S[/itex]
[itex]ds^b ds_b=ds^2[/itex]

As @haushofer said, both equations use the same metric.
The first equation is an equality of scalar fields, the d’Alembertian of a scalar field [itex]u[/itex] and a scalar field [itex]S[/itex] .
The second equation is an infinitesimal scalar [at a point] using the RHS as an abbreviation of the LHS.
 
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