Let $I$ be a finite, countably infinite or uncountable index set and let $(\Omega_i,\mathcal{A}_i)_{i \in I}$ be measurable spaces. Then we can define the sigma algebra
$$ \mathcal{A} := \bigotimes_{i \in I} \mathcal{A}_i $$
on the product space $\Omega := \times_{i \in I} \Omega_i$ as the smallest sigma algebra, such that all projections $$ \pi_i\rightarrow \Omega : \Omega_i, \quad \omega \mapsto \omega_i, $$ are $\mathcal{A}$-$\mathcal{A}_i$-measurable.
This is the canonical way of defining a $\sigma$-algebra on a product space and is used (mostly without further explanation) in lots of textbooks about advanced probability.
My problem is that I am lacking intuitive motivation for this defintion. Is this the only reasonable way to define a $\sigma$-algebra on the product space? Why? If not, why do whe choose this definition over all other possible methods for constructing $\sigma$-algebras on $\Omega$? What are the essential advantages of this definition? In short: why is this the right $\sigma$-algebra on $\Omega$? Why could it not be different?
Kind regards and thanks for any help!
Let $(\Omega',\mathcal A')$ be a measurable space and let $f_i:\Omega'\to\Omega_i$ for $i\in I$ denote a collection of measurable maps.
Then especially if $\Omega$ is equipped with $\mathcal A=\bigotimes_{i \in I} \mathcal{A}_i$ a unique measurable $f:\Omega'\to\Omega$ such the $f_i=\pi_i\circ f$ for every $i\in I$.
Conversely every measurable map $f:\Omega'\to\Omega$ induces a family $\{f_i=\pi\circ f:\Omega'\to\Omega_i\mid i\in I\}$ of measurable maps, so the correspondence is one-to-one.
This offers the nice possibility to identify families $\{f_i\mid i\in I\}$ of measurable maps that have common domain with just one measurable map $f$.
That is for a good deal the underlying motivation for the construction of products.