The Euler characteristic behaves well with respect to many basic operations on topological spaces, as follows.
Homotopy invariance Homology is a topological invariant, and moreover a
homotopy invariant: Two topological spaces that are
homotopy equivalent have
isomorphic homology groups. It follows that the Euler characteristic is also a homotopy invariant. For example, any
contractible space (that is, one homotopy equivalent to a point) has trivial homology, meaning that the 0th Betti number is 1 and the others 0. Therefore, its Euler characteristic is 1. This case includes
Euclidean space \mathbb{R}^n of any dimension, as well as the solid unit ball in any Euclidean space — the one-dimensional interval, the two-dimensional disk, the three-dimensional ball, etc. For another example, any convex polyhedron is homeomorphic to the three-dimensional
ball, so its surface is homeomorphic (hence homotopy equivalent) to the two-dimensional
sphere, which has Euler characteristic 2. This explains why the surface of a convex polyhedron has Euler characteristic 2.
Inclusion–exclusion principle If
M and
N are any two topological spaces, then the Euler characteristic of their
disjoint union is the sum of their Euler characteristics, since homology is additive under disjoint union: :\chi(M \sqcup N) = \chi(M) + \chi(N). More generally, if
M and
N are subspaces of a larger space
X, then so are their union and intersection. In some cases, the Euler characteristic obeys a version of the
inclusion–exclusion principle: :\chi(M \cup N) = \chi(M) + \chi(N) - \chi(M \cap N). This is true in the following cases: • if
M and
N are an
excisive couple. In particular, if the
interiors of
M and
N inside the union still cover the union. • if
X is a
locally compact space, and one uses Euler characteristics with
compact supports, no assumptions on
M or
N are needed. • if
X is a
stratified space all of whose strata are even-dimensional, the inclusion–exclusion principle holds if
M and
N are unions of strata. This applies in particular if
M and
N are subvarieties of a
complex algebraic variety. In general, the inclusion–exclusion principle is false. A
counterexample is given by taking
X to be the
real line,
M a
subset consisting of one point and
N the
complement of
M.
Quotient space If
X is a finite CW-complex and
A is a subcomplex, then :\chi(X) = \chi(A) + \chi(X/A) -1. The formula could be more succinctly written for the reduced Euler characteristic—the alternating sum of ranks of reduced homology groups.
Connected sum For two connected closed
n-manifolds M, N one can obtain a new connected manifold M \mathbin{\#} N via the
connected sum operation. The Euler characteristic is related by the formula : \chi(M \mathbin{\#} N) = \chi(M) + \chi(N) - \chi(S^n).
Product property Also, the Euler characteristic of any
product space M ×
N is :\chi(M \times N) = \chi(M) \cdot \chi(N). Using this and the formula for quotient spaces, one obtains :\hat\chi(M \wedge N) = \hat\chi(M) \cdot \hat\chi(N), where \hat\chi is the reduced Euler characteristic, and M\wedge N is the
smash product. These addition and multiplication properties are also enjoyed by
cardinality of
sets. In this way, the Euler characteristic can be viewed as a generalisation of cardinality; see .
Covering spaces Similarly, for a
k-sheeted
covering space \tilde{M} \to M, one has :\chi(\tilde{M}) = k \cdot \chi(M). More generally, for a
ramified covering space, the Euler characteristic of the cover can be computed from the above, with a correction factor for the ramification points, which yields the
Riemann–Hurwitz formula.
Fibration property The product property holds much more generally, for
fibrations with certain conditions. If p\colon E \to B is a fibration with fiber
F, with the base
B path-connected, and the fibration is orientable over a field
K, then the Euler characteristic with coefficients in the field
K satisfies the product property: :\chi(E) = \chi(F)\cdot \chi(B). This includes product spaces and covering spaces as special cases, and can be proven by the
Serre spectral sequence on homology of a fibration. For fiber bundles, this can also be understood in terms of a
transfer map \tau\colon H_*(B) \to H_*(E) – note that this is a lifting and goes "the wrong way" – whose composition with the projection map p_*\colon H_*(E) \to H_*(B) is multiplication by the
Euler class of the fiber: :p_* \circ \tau = \chi(F) \cdot 1. ==Examples==