We present a possible generalization of the exterior differential calc
ulus, based on the operator d such that d(3) = 0, but d(2) not equal 0
. The entities dx(i) and d(2)x(k) generate an associative algebra; we
shall suppose that the products dx(i) dx(k) are independent of dx(k) d
x(i), while the ternary products will satisfy the relation: dx(i) dx(k
) dx(m) = j dx(k) dx(m) dx(i) = j(2)dx(m) dx(i) dx(k), complemented by
the relation dx(i) d(2)x(k) = jd(2)x(k)dx(i), with j := e(2 pi i/3).
We shall attribute grade 1 to the differentials dx(i) and grade 2 to t
he 'second differentials' d(2)x(k); under the associative multiplicati
on law the grades add up module 3. We show how the notion of covariant
derivation can be generalized with a 1-form A so that D Phi := d Phi
+ A Phi, and we give the expression in local coordinates of the curvat
ure 3-form defined as Omega := d(2)A + d(A(2)) + A dA + A(3). Finally,
the introduction of notions of a scalar product and integration of th
e Z(3)-graded exterior forms enables us to define the variational prin
ciple and to derive the differential equations satisfied by the 3-form
Omega. The Lagrangian obtained in this way contains the invariants of
the ordinary gauge field tensor F-ik and its covariant derivatives Di
Fkm.