For a two-dimensional incompressible flow , the continuity equation is . Locally, or globally on a simply connected fluid region, this permits a streamfunction with
Indeed, the one-form is closed by incompressibility and hence is locally the differential of . Conversely these expressions automatically give zero divergence by equality of mixed derivatives.
A streamline at a fixed time is tangent to the instantaneous velocity field. Along it,
Thus streamlines are connected curves on which the streamfunction is constant; wherever , the level curves have exactly the required tangent direction. At a stagnation point, the tangent is degenerate and distinct branches of a level set need not form a single streamline. For unsteady flow this argument fixes time: it does not identify streamlines with particle pathlines.

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