Topological manifold Created 2026-09-24 Updated 2026-10-14
A topological -manifold without boundary is a topological space satisfying three conditions: it is Hausdorff, it is second countable, and every point lies in an open set with a homeomorphism onto an open set . Here is a fixed dimension of a manifold, and has the usual topology of Euclidean space. The pair is a coordinate chart. Unless explicitly qualified, “topological manifold” here means without boundary.[ref]
The Hausdorff condition requires disjoint open neighbourhoods for distinct points. Second countability requires a countable basis of a topology. Neither follows merely from the local homeomorphisms: non-Hausdorff manifolds fail the first condition, while an uncountable disjoint union of copies of the real line fails the second. Indeed, a basis of a topology must supply a different nonempty member inside each copy, so it cannot be countable.
The circle and the real line are both one-dimensional topological manifolds, with the same local model. Their global topologies differ: the circle is compact, while the real line is not. By contrast, the junction of a topological tripod already fails the local test. Thus local coordinate charts specify what kind of small pieces are allowed; global topological invariants distinguish how those pieces fit together.[ref]
The usefulness of a topological manifold is that local questions about continuity can be transported into Euclidean space, while compactness, connectedness, and the fundamental group still record global information. For calculus, further structure is needed: a smooth atlas requires smooth transition maps, letting the chain rule reconcile derivatives computed in different coordinate charts. A topological atlas by itself only guarantees homeomorphisms between coordinates.[ref]
Take the circle with its subspace topology. Write for its west point and for its east point. Two coordinate charts obtained by stereographic projection are
Both take values in the entire real line. Geometrically, join to and intersect the resulting line with : the height is . Projecting from instead gives height . Each projection omits its own starting point, but the other coordinate chart includes that point. Hence .[ref]
Figure 1.
Two stereographic charts cover the circle and unfold it onto two real lines
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To verify the homeomorphisms, solve the displayed equations for . The inverse functions are
Each formula lies on the circle, avoids its excluded point, and is continuous for every real argument. Substitution into the projection formulas returns or ; substitution in the other direction returns . Thus these are continuous bijections with continuous inverse functions, as required for coordinate charts. Since the Euclidean plane is Hausdorff and second countable, the subset with its subspace topology is too. This checks all three conditions for a topological manifold, rather than just drawing a smooth-looking curve.
On the overlap , both are excluded, so . Using , the topological transition map is
For example, has and . The two connected components of the overlap, the upper and lower arcs, correspond to the positive and negative parts of the punctured real line. The values and represent and , respectively, and belong to only one chart each. The reciprocal coordinate change and its inverse function are smooth functions away from zero, so this topological atlas also supplies a smooth atlas.
Why can neither chart be enlarged to a single coordinate chart on the whole circle? The circle is a closed set and a bounded set in the Euclidean plane, hence compact by the Heine-Borel theorem. A global coordinate chart would give a homeomorphism to a nonempty open set . Its image would be compact and therefore closed in the real line. By connectedness of the real line, this forces , which is not compact. This is the one-dimensional instance of no compact manifold has a single Euclidean chart. Locally the circle is indistinguishable from the real line; globally compactness obstructs a single chart.