The following appears in ANALYTICAL MECHANICS Classical, Lagrangian and Hamiltonian Mechanics, Stability Theory & Special Relativity, by Valter Moretti
Definition 1.22 A differentiable manifold of dimension $n$ and class $\mathcal{C}^{k}$, for given $n\in\left\{ 1,2,3,\dots\right\} $ and $k\in\left\{ 1,2,3,\dots\right\} \cup\left\{ \infty\right\} $, is a locally Euclidean, Hausdorff and second countable topological space $M$, whose elements are called points, equipped with a differentiable structure of class $\mathcal{C}^{k}$ and dimension $n$. The differentiable structure is a collection of $n$-dimensional local charts $\mathcal{A}=\left\{ \left(U_{i},\phi_{i}\right)\right\} _{i\in I}$ satisfying the following:
(1) $\cup_{i\in I}U_{i}=M;$
(2) the local charts in $\mathcal{A}$ must be pairwise $\mathcal{C}^{k}$ -compatible;
(3) $\mathcal{A}$ is maximal with respect to (ii): if $\left(U,\phi\right)$ is an $n$-dimensional local chart on $M$ compatible with every chart of $\mathcal{A}$, then $\left(U,\phi\right)\in\mathcal{A}.$
It is evident that the statement of item (3) of this definition is not what was intended. I have contacted the author, but I suspect he appropriately is busy with paying students. How might this definition be amended so that it is coherent and correct? There is nothing in the context labeled "(ii):".
I'm thinking it should be something like:
(3) (i) $\mathcal{A}$ is maximal with respect to $M;$
(ii) if $\left(U,\phi\right)$ is an $n$-dimensional local chart on $M$ compatible with every chart of $\mathcal{A}$, then $\left(U,\phi\right)\in\mathcal{A}.$
Even if my suggested (3)(i) is correct, I am still unsure about (3)(ii).
This notion of maximality regarding charts and atlases (my term) is unfamiliar to me.
– Steven Thomas Hatton Jan 07 '25 at 20:33