There isn't.
Torsion represents the failure of "infinitesimal parallelograms" to close.
To see this, consider a point $x$ and and two "infintesimally nearby" points $x_1^\mu=x^\mu+\frac{dx^\mu}{d\tau}d\tau=x^\mu+T^\mu d\tau$ and $x_2^\mu =x^\mu+S^\mu d\sigma$.
Now we parallel transport $T^\mu d\tau$ to the second point $x^\mu+S^\mu d\sigma$:
$$ T^\mu(x_2)d\tau=(T^\mu-\Gamma^\mu_{\nu\sigma}S^\nu d\sigma T^\sigma) d\tau, $$ add this to the second point and get $$x_3^\mu= x^\mu +S^\mu d\sigma+T^\mu d\tau-\Gamma^\mu_{\nu\sigma}S^\nu T^\sigma d\sigma d\tau. $$
What if we do the other way around and transport $S^\mu d\sigma$ to $x_1$?
We get $$ \tilde{x}_3^\mu=x^\mu+T^\mu d\tau+S^\mu d\sigma-\Gamma^\mu_{\nu\sigma}T^\nu S^\sigma d\sigma d\tau. $$
The difference of these two points is $$\Delta x_3^\mu=(\Gamma^\mu_{\nu\sigma}-\Gamma^\mu_{\sigma\nu})d\sigma d\tau=T^\mu_{\ \nu\sigma}d\sigma d\tau.$$
The reason I say that is to illustrate that the core concept of torsion involves parallel transporting one vector along another, and then doing the same operation in reverse, transporting the "other" vector along the former one. The invariant definition $$ T(X,Y)=\nabla_XY-\nabla_YX-[X,Y] $$also implies this.
For a general connection, the direction of parallel transport is given by a vector, but the object to be parallel transported are not vectors but general fiber elements. So the operation of transporting a fiber element along a vector, and then transporting the vector along a fiber element makes no sense, because a fiber element doesn't determine a direction in the manifold in general. Eg. the expression $D_Xs$ cannot be symmetrized or antisymmetrized, since $X$ and $s$ are very different objects.
Curvature doesn't have the same problem, since there two vectors are needed to generate a loop, but only a fiber element gets transported.