ConceptComplete

Van Kampen's Theorem - Examples and Constructions

The power of Van Kampen's theorem lies in its applications to concrete computations. We examine key examples that illustrate the technique.

Example

Fundamental group of the torus: Write T2T^2 as a square with opposite sides identified. Decompose T2=UVT^2 = U \cup V where:

  • UU is the torus minus a point (deformation retracts to a figure-eight)
  • VV is a small disk around the removed point (contractible)
  • UVU \cap V deformation retracts to S1S^1

Then π1(U)ZZ\pi_1(U) \cong \mathbb{Z} * \mathbb{Z}, π1(V)={e}\pi_1(V) = \{e\}, and π1(UV)=Z\pi_1(U \cap V) = \mathbb{Z}. The inclusion UVUU \cap V \to U corresponds to the commutator [a,b][a,b] in the free group. Van Kampen gives: π1(T2)a,b[a,b]=1=Z×Z\pi_1(T^2) \cong \langle a, b \mid [a,b] = 1 \rangle = \mathbb{Z} \times \mathbb{Z}

This computation reveals the abelian structure of π1(T2)\pi_1(T^2), reflecting the fact that loops on the torus commute.

Example

Orientable surfaces of genus gg: The surface Σg\Sigma_g can be decomposed as Σg=Σg1disk(torus minus disk)\Sigma_g = \Sigma_{g-1} \cup_{\text{disk}} (\text{torus minus disk}). Iteratively applying Van Kampen: π1(Σg)a1,b1,,ag,bg[a1,b1][ag,bg]=1\pi_1(\Sigma_g) \cong \langle a_1, b_1, \ldots, a_g, b_g \mid [a_1,b_1] \cdots [a_g,b_g] = 1 \rangle This is a 2g2g-generated group with one relation, showing the rich structure of surface fundamental groups.

Example

Complement of knots: For a knot KS3K \subseteq S^3, decompose S3K=UVS^3 \setminus K = U \cup V where UU is a tubular neighborhood of KK (with π1Z\pi_1 \cong \mathbb{Z}) and VV is the exterior. Van Kampen relates the knot group π1(S3K)\pi_1(S^3 \setminus K) to the structure of UVU \cap V, a torus. This gives: π1(S3K)generatorsWirtinger relations\pi_1(S^3 \setminus K) \cong \langle \text{generators} \mid \text{Wirtinger relations} \rangle

The Wirtinger presentation can be read directly from a knot diagram, making Van Kampen a practical computational tool in knot theory.

Example

Real projective spaces: Write RPn=UV\mathbb{RP}^n = U \cup V where UU is a contractible neighborhood of a point and VV is a neighborhood of the complement, deformation retracting to RPn1\mathbb{RP}^{n-1}. Then UVSn1U \cap V \simeq S^{n-1}, and for n3n \geq 3: π1(RPn)π1(RPn1){e}{e}=π1(RPn1)\pi_1(\mathbb{RP}^n) \cong \pi_1(\mathbb{RP}^{n-1}) *_{\{e\}} \{e\} = \pi_1(\mathbb{RP}^{n-1}) By induction from π1(RP2)=Z/2Z\pi_1(\mathbb{RP}^2) = \mathbb{Z}/2\mathbb{Z}, we get π1(RPn)Z/2Z\pi_1(\mathbb{RP}^n) \cong \mathbb{Z}/2\mathbb{Z} for all n2n \geq 2.

Remark

Van Kampen's theorem is most powerful for CW complexes and spaces built by attaching cells. The attaching maps translate directly into relations in the fundamental group presentation, making the algebraic structure explicit.

Example

Bouquet of circles: The wedge sum of nn circles has π1=Fn\pi_1 = \mathbb{F}_n, the free group on nn generators. This follows from iteratively applying Van Kampen with trivial overlaps. The figure-eight is F2=a,b\mathbb{F}_2 = \langle a, b \mid \rangle.

These examples demonstrate that Van Kampen's theorem reduces fundamental group computations to combinatorial group theory, making previously intractable problems solvable.