*Let K be a field and L an extension of K generated by an element x such that x∈/K, xp∈K. Let V be a vector space over L and A a derivation of K into V such that Δ(xp)=0. Then there exists a unique derivation D of L into V extending A and such that D(x)=0.
By V, p. 24, Prop. 1, {1, x, …, xp−1} is a basis of L over K. For every element u=a0+a1x+…+ap−1xp−1 of L (with a0, …, ap−1 in K) we put D(u)=A(a0)+xΔ(a1)+…+xp−1Δ(ap−1). It is clear that D extends A and satisfies (1); so it is enough to establish the relation
D(uv)=u⋅D(v)+v⋅D(u)
when u is of the form axi and v of the form bxj with a, b in K, 0≤i<p and 0≤j<p.
When i+j<p we have uv=xi+jab, whence D(uv)=xi+jΔ(ab). Otherwise we have 0≤i+j−p<p and so uv=xi+j−p(abxp), with abxp∈K, but since A(xp)=0, we have A(abxp)=xpA(ab), whence again D(uv)=xi+jΔ(ab). So we have in all cases
D(uv)=xi+jΔ(ab)=xixj(a⋅A(b)+b⋅Δ(a))=(axi)xj⋅Δ(b)+(bxj)xi⋅Δ(a)=u⋅D(v)+v⋅D(u).
Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.
Nothing.