Let n,k∈N with k≤n, let (S,ε) be an oriented k-sub-rectangle of Rn, let U⊆Rn be open with S⊆U, and let ω be a continuous differential k-form on U. Choose data as in Oriented k-Sub-Rectangle of Euclidean Space, so that S=λR(R) for a standard k-rectangle
R=[a1,b1]×⋯×[ak,bk]
and active coordinate indices 1≤i1<⋯<ik≤n. Write ω in the coordinate expansion from Coordinate Expansion of Differential Forms on Euclidean Open Sets. Let f:U→R be the coefficient function of the basis form
dxi1∧⋯∧dxik.
For each fixed (t2,…,tk)∈[a2,b2]×⋯×[ak,bk], define
F1(t2,…,tk)=∫a1b1f(λR(t1,t2,…,tk))dt1,
where this is the one-dimensional Riemann integral on [a1,b1]; it exists because the integrand is continuous on [a1,b1], hence Riemann integrable. Recursively, for each r∈{2,…,k} and each fixed (tr+1,…,tk)∈[ar+1,br+1]×⋯×[ak,bk], define
Fr(tr+1,…,tk)=∫arbrFr−1(tr,…,tk)dtr,
again in the one-dimensional Riemann sense of The Riemann Integral on a Closed Interval via Lower and Upper Integrals, whenever the integrand is viewed as a function of tr alone. The integral of ω over (S,ε) is defined by
∫(S,ε)ω=εFk.
Equivalently,
∫(S,ε)ω=ε∫akbk⋯∫a1b1f(λR(t1,…,tk))dt1⋯dtk,
with the right-hand side understood through the recursive construction above.