For three-momentum , force and acceleration satisfy
The associated four-force uses proper time instead of coordinate time and is a different, four-dimensional object.
The three-force measured in a particle's instantaneous rest frame. For a pure force, , where is the rest-frame acceleration. In that frame the four-force has zero temporal component and spatial part ; the four-force itself is a different object.
Under a constant force with , momentum is and
The speed approaches without reaching it at finite time.

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