If $F_\nabla$ is the curvature associated to a connection $\nabla$ on a 2-dimensional Riemannian manifold $M$ with metric $g$, then we can define ''the'' Riemann curvature by (https://en.wikipedia.org/wiki/Curvature_of_Riemannian_manifolds) by $$ R(X,Y,Z,W) = g(F_\nabla (X,Y)Z, W) $$ for vector fields $X,Y,Z,W$. This is related to a function $K: M\to \mathbb{R}$ by $$ K(x)\sigma(X,Y)\sigma(Z,W) = R(X,Y,Z,W)\mid_x $$ where $\sigma = e_1^{*}\wedge e_2^*$ is a globally-defined non-vanishing 2-form, and $e_1^*, e_2^*$ are dual to an orthonormal frame $e_1, e_2$. (Side note: is this function the same as the sectional curvature?)
What I would like to understand is whether there is a more direct way to express $K$ in terms of $g$ and $F_\nabla$: for example, a dual section $s^*$ is defined by $s^{*} = g(s,\cdot)$ - so can we say something like $$ K(x)\sigma = \langle\omega , e_1\wedge e_2\rangle\mid_x $$ where $\omega(s_1, s_2) := g(F_\nabla s_1, s_2)$ for vector fields $s_1, s_2$, and $\langle \cdot, \cdot\rangle$ in this instance is meant to indicate the natural pairing of a 2-form with a bivector.