The better methods will depend upon the voltage difference you are attempting to measure. Same would be true for your hydraulic analogy.
But your hydraulic analogy fails entirely in another regard. The accelerating forces acting on electrons in a conductor are caused by very few charges. I don't think you have a feel for just how few electrons are needed at the surface of a conductor to accelerate significant mean-velocities for charges in a wire. If you bend a wire into a U-shape, it might only take one or two extra electrons at the bend to completely re-direct amps of current.
You can measure high voltage differences because the amount of charge difference reaches the point where sensitive (pith balls on a hair-like thread, for example) can be applied successfully. In this case, the impact on current is just as negligible as your hydraulic example's momentary impact due to very slight piston flexures.
For small voltages, this doesn't work because the charge difference is so absolutely tiny and any finite distance away from the bare conductor surface greatly reduces the tiny force.
The electronic equivalent to hydraulic pressure is \$\frac{\textrm{volts}}{\textrm{meter}}\$ or \$\frac{\textrm{Newton}}{\textrm{Coulomb}}\$. Copper's conduction electron density at room temperature is about \$1.346\times 10^{10}\:\frac{\textrm{Coulomb}}{\textrm{m}^3}\$ and their mobility is about \$4.5\times 10^{-3}\:\frac{\textrm{m}^2}{\textrm{V-s}}\$. Assume a wire with a cross-section of \$1\:\textrm{mm}^2\$ and carrying \$300\:\textrm{mA}\$ of current. The electric field required is about \$5\:\frac{\mu\textrm{V}}{\textrm{mm}}\$.
The charge difference over reasonable distances needed to impel that current is negligible (which resides entirely on the bare surface of the conductor) and you wouldn't be able to set up an instrument to measure it at any finite distance away. The only way to make this work is to add a conductor to the surface of that other conductor at some point and allow these tiny charge differences to act on their atomic scales so that their incredible forces can impel electrons in your measurement instrument as well. In short, you need to allow a current to flow, because this IS the most sensitive way available to you (at non-military budget levels) to make those pressure measurements in electronics.
It's nice to think about analogies, of course. But as you already know, the scale also matters. There's a huge difference between the distances separating galaxies and the forces that meaningfully act at that level and the distances separating atoms and the forces that meaningfully act at that level. Put in a more tactile level we humans can think in terms of, there's a huge difference between the forces that are important to us for walking and getting traction and the forces that act on fruit flies, who can easily land on the surfaces of walls and the ceiling because gravity is far less important at their scale compared to static charge and roughness for them.
Scale matters, too.
So the analogy fails here. In electronics, the very best way to measure these extremely delicate and tiny forces, which are all that is needed to impel practical currents in circuits, is to set up a measurement system that can respond to them. This means allowing a current to be affected. There's nothing more sensitive than that.
That said, I'll return to the fact that you can still make measurements without a current if and only if the voltage differences are large enough to set up enough charge difference to measure.