# Minkowski spacetime

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Since *ds* is frame independent we can interpret this result geometrically by treating points in the four dimensional spacetime, with *ds* representing the four dimensional distance [ interval ] between neighboring points.

The expression for *ds* looks Euclidian if the time component is taken to be *ict*, :

The line element allows one to classify spacetime intervals into three different classes: Consider a curve [ world- line of a particle, say] and an interval on that curve. If:

the curve is timelike in that interval;

the curve is spacelike in that interval; and

the curve is null in that interval.

Note that the sign of is a matter of convention, invariance between frames is what is important.