Let RR be a ring, let

0⟶A′→uA→vA′′⟶00 \longrightarrow A' \xrightarrow{u} A \xrightarrow{v} A'' \longrightarrow 0

be a of right RR-modules, and let BB be a left RR-module. Then there are natural connecting homomorphisms

δn:Tor⁡nR(A′′,B)⟶Tor⁡n−1R(A′,B)(n≥1),\delta_n:\operatorname{Tor}_n^R(A'',B)\longrightarrow \operatorname{Tor}_{n-1}^R(A',B) \quad (n\ge 1),

(see ) such that the following sequence is exact:

⋯→Tor⁡2R(A′′,B)→δ2Tor⁡1R(A′,B)→Tor⁡1R(A,B)→Tor⁡1R(A′′,B)→δ1A′⊗RB→A⊗RB→A′′⊗RB→0.\cdots \to \operatorname{Tor}_2^R(A'',B)\xrightarrow{\delta_2}\operatorname{Tor}_1^R(A',B)\to \operatorname{Tor}_1^R(A,B)\to \operatorname{Tor}_1^R(A'',B) \xrightarrow{\delta_1} A'\otimes_R B \to A\otimes_R B \to A''\otimes_R B \to 0.

Equivalently, for every n≥1n\ge 1 one has exactness at the three-term window

Tor⁡nR(A′,B)⟶Tor⁡nR(A,B)⟶Tor⁡nR(A′′,B)→δnTor⁡n−1R(A′,B).\operatorname{Tor}_n^R(A',B)\longrightarrow \operatorname{Tor}_n^R(A,B)\longrightarrow \operatorname{Tor}_n^R(A'',B)\xrightarrow{\delta_n}\operatorname{Tor}_{n-1}^R(A',B).

This is a special case of the general .

Examples
  1. Computing Tor⁡1Z(Z/n,Z/m)\operatorname{Tor}_1^{\mathbb Z}(\mathbb Z/n,\mathbb Z/m). Use the short exact sequence
    0→Z→⋅nZ→Z/n→0.0\to \mathbb Z \xrightarrow{\cdot n}\mathbb Z \to \mathbb Z/n \to 0.
    Tensor with Z/m\mathbb Z/m. Since Z⊗Z/m≅Z/m\mathbb Z\otimes \mathbb Z/m\cong \mathbb Z/m, the relevant part of the long exact sequence becomes
    0→Tor⁡1Z(Z/n,Z/m)→Z/m→⋅nZ/m→(Z/n)⊗Z/m→0.0 \to \operatorname{Tor}_1^{\mathbb Z}(\mathbb Z/n,\mathbb Z/m) \to \mathbb Z/m \xrightarrow{\cdot n} \mathbb Z/m \to (\mathbb Z/n)\otimes \mathbb Z/m \to 0.
    Hence
    Tor⁡1Z(Z/n,Z/m)≅ker⁡(⋅n:Z/m→Z/m)≅Z/gcd⁡(n,m).\operatorname{Tor}_1^{\mathbb Z}(\mathbb Z/n,\mathbb Z/m)\cong \ker(\cdot n:\mathbb Z/m\to \mathbb Z/m)\cong \mathbb Z/\gcd(n,m).
    (Also Tor⁡iZ(Z/n,−)=0\operatorname{Tor}_i^{\mathbb Z}(\mathbb Z/n,-)=0 for i≥2i\ge 2 because Z/n\mathbb Z/n has a length-1 projective resolution.)
  1. Over a field, higher Tor vanishes. If R=kR=k is a field and V,WV,W are kk-vector spaces, then VV is free (hence projective), so Tor⁡ik(V,W)=0\operatorname{Tor}_i^k(V,W)=0 for all i≥1i\ge 1. The long exact sequence above reduces to exactness of
    0→V′⊗kW→V⊗kW→V′′⊗kW→0,0\to V'\otimes_k W \to V\otimes_k W \to V''\otimes_k W \to 0,
    reflecting that −⊗kW-\otimes_k W is exact.
  1. Dual numbers. Let R=k[ε]/(ε2)R=k[\varepsilon]/(\varepsilon^2) and regard k=R/(ε)k=R/(\varepsilon) as an RR-module. The periodic free resolution
    ⋯→⋅εR→⋅εR→⋅εR⟶k⟶0\cdots\xrightarrow{\cdot\varepsilon}R\xrightarrow{\cdot\varepsilon}R \xrightarrow{\cdot\varepsilon}R\longrightarrow k\longrightarrow0
    becomes a complex with zero differentials after tensoring with kk. Hence
    Tor⁡iR(k,k)≅k(i≥1).\operatorname{Tor}_i^R(k,k)\cong k\qquad(i\ge1).