Consider the manifold $(\mathbb{R}^{2}, \mathcal{O})$ (where $\mathcal{O}$ is the standard topology on $\mathbb{R}^{2}$) be equipped with the atlas $\mathcal{A} = \{(\mathbb{R}^{2}, x), (\mathbb{R}^{2}, y)\}$ such that $x: \mathbb{R}^{2} \to \mathbb{R}^{2}$, where $x(a,b) := (a,b)$, and $y: \mathbb{R}^{2} \to \mathbb{R}^{2}$ where $y(a,b) : =(a,b + a^{3})$.
We are asked to compute the $(\text{dim}\mathbb{R}^{2})^{2} = 4$ objects $\left(\frac{\partial x^{i}}{\partial y^{j}}\right)_{p} := \partial_{j}(x^{i} \ \circ \ y^{-1})(y(p))$.
I found the inverse of $y$ to be defined as $y^{-1}(u,v) = (u, v-u^{3})$ and so we have $x^{i} \ \circ \ y^{-1} : \mathbb{R^{2}} \to \mathbb{R}$ where using the chart map $x$ we have $(x \ \circ \ y^{-1})(u,v) = (u, v-u^{3})$. In the solution for $\left(\frac{\partial x^{2}}{\partial y^{1}}\right)_{p}$, for example, the author says to differentiate $x^{2}$ (the second component function of $x$) with respect to the first entry (which in this case would be the symbol $u$) which he claims would give us
$$\partial_{1}(x^{2} \ \circ \ y^{-1})(a, b+a^{3}) = -3u^{2} = -3a^{2}. (*)$$
However, in the video, there's a lot of steps skipped and I can't seem to understand how he arrived at this solution. Do we have to perform the multidimensional chain rule for each $\left(\frac{\partial x^{i}}{\partial y^{j}}\right)_{p}$? I.e., maybe for the example above, if $$h(a, b+a^{3}) := x^{2}(y^{-1}(a, b+a^{3})) $$ then (writing something like the following, where $u=a$, $v = b+a^{3}$) $$Dh(u,v) = Dx^{2}(y^{-1}(u,v)))Dy^{-1}(u,v)?$$
If someone could please walk me through these steps or show me that I'm completely overthinking it would be greatly appreciated.
$(*)$ Another thought: It seems like, since $x$ is the identity function on $\mathbb{R}^{2}$, we don't need to use the chain rule explicitly and can just take the partial derivative of $x^{i}$ with respect to either $u$ or $v$.