Ibix said:
Fair point. So what would you suggest as the origin of force as a concept? It remains the rate of change of four momentum, and fouromentum is a normalised tangent to the worldline, but why is that normalisation of interest?
Indeed, "a force", seems to be best defined by the equation of motion of a particle in an external field,
$$\mathrm{d}_{\tau} p^{\mu}=F^{\mu}(x,p), \quad \mathrm{d}_{\tau} x^{\mu}=\frac{1}{m} p^{\mu},$$
where ##m## is the invariant mass. The "Minkowski force" ##F## must obey the contraint
$$p_{\mu} F^{\mu}=0,$$
such that the equation of motion is consistent with
$$p_{\mu} p^{\mu}=m^2 c^2 =\text{const}.$$
Of course, all this even holds within GR. Then you only have to use the covariant derivative wrt. ##\tau##,
$$\mathrm{D}_{\tau} p^{\mu} = \mathrm{d}_{\tau} p^{\mu} + {\Gamma^{\mu}}_{\rho \sigma} p^{\rho} \mathrm{d}_{\tau} x^{\sigma}.$$
Note that then on the right-hand side you only have the forces but not gravity, which is contained on the left-hand side of the equation. In GR gravity is not a force to begin with of course. Perhaps it's anyway best to first concentrate on SRT only, excluding the discussion of gravity at this stage...