I would like to show that $\dot\partial \wedge P(\dot{a}) = P(\partial \wedge a)$, where $P$ is a linear function $P(a(x)) = a(x)\cdot I(x)I^{-1}(x)$. The dot is used to indicate that the derivative is acting only on $a$, not on the $I$'s.
Note that $I$ is a pseudoscalar of a lower dimensional manifold that lives in a larger dimensional ambient space. The vector $a$ is also in the lower dim manifold. In general, $\partial \wedge a(x)$ has a component that is outside the manifold, and a component that is inside the manifold. This fact might be coming into play. For more context, the claim in Doran and Lasenby (pg 210) is that
$$ \partial \wedge a = \partial \wedge (P(a)) = \dot \partial \wedge \dot{P}(a) + P(\partial \wedge a) = \dot{\partial} \wedge \dot{P}(a) + D\wedge a $$
What I would like to prove is the unspoken part where $\dot \partial \wedge P(\dot{a})=P(\partial \wedge a)$.
Attempt: \begin{align*} \dot\partial \wedge P(\dot{a}) &= \langle \dot\partial \wedge (\dot a\cdot II^{-1}) \rangle_2 \\ &= \langle \dot\partial (\dot{a}I - \dot{a}\wedge I) I^{-1} \rangle_2 \\ &= \langle \dot\partial \dot{a}I) I^{-1} \rangle_2 \\ &= \langle \dot \partial \dot{a}\rangle_2 \\ &= \partial \wedge a \quad \textrm{(wrong)} \end{align*}
Equation (6.199), page 204 of Doran and Lasenby: $$ P(\partial) = \partial. $$ This is because $\partial$ is the tangential derivative that only differentiates along directions tangential to the manifold. It then follows simply that $$ \dot\partial\wedge P(\dot a) = P(\dot\partial)\wedge P(\dot a) = P(\dot\partial\wedge\dot a). $$