It seems 1-form on a manifold (let's limit our discussion to be a 2-manifold) is derivative $d\eta$ of a function $\eta:M\rightarrow \mathbb{R}$. It's similar to the derivative of $f:\mathbb{R}^2\rightarrow \mathbb{R}$, i.e. $df=df(x)=f'(x)dx$, which is in diff geom notation, $df_x(dx)$, a linear approximation of change of $f$'s value at point $x$ with displacement dx. (right?)
Then what's the analog of 2-form for $f:\mathbb{R}^2\rightarrow \mathbb{R}$? e.g. something like $\int\int f_xf_ydxdy+f_yf_xdydx+f_xf_xdxdx+f_yf_ydydy$ ($f_x$ etc. mean partial derivative)?
(Edited to add:)
This section is a note for myself:
Since a 2-form can be derived from 1-form $\omega$ in the following way:
$X(\omega Y)+Y(\omega X)+\omega[X,Y]$
all three items are like '1-form times or acting on a vector field', I guess 2-form would be like (especially when $\omega$ is exact), or more specifically like a linear combination of differential (in Lie derivative sense; by Lie derivative we get sth of the same kind) of
$$\sum \frac{\partial f}{\partial x^i} (\sum a^i\frac{\partial }{\partial x^j}).$$
Since 2-form is a (covariant tensor) field, its value at a point $p$ will be like
$$\sum (\frac{\partial }{\partial x^i})_p\ f \cdot (\sum (a^j)_p(\frac{\partial }{\partial x^j})_p),$$
where ${x^I}_p$ is the coordinate system at $p$.
So to understand 2-form perhaps I need to understand vector field/tangent bundle and its basis as well as Lie derivative, and do some calculation about them in a coordinate system.