In my physics education, we did labs with traditional equipment to better learn the fundamentals.
This included bridges of various types, including Wheatstone and Kelvin, and "potentiometers" (in the literal meaning of the word) to measure voltage.
The coolest galvanometers were the ones firmly mounted to a concrete wall.
To read them, one attached a scale on an arced surface with a telescope mounted above it, to see the numbers reflected off the mirror in the galvanometer.
(Of course, the numbers were reversed on the scale to read properly after reflection.)
Used as "ballistic galvanometers", where one read the maximum excursion and calculated knowing the mechanical parameters of the instrument, these could measure charge directly.
Used normally, they gave a very sensitive null indication, with no bias current.
In "Vacuum Tube Amplifiers" (Radiation Laboratory Series Vol 18), ed G E Valley and H Wallman, McGraw-Hill 1948, pp 490-491, there is a simple DC amplifier using a dual phototube (920) illuminated by such a galvanometer, driving a simple 6SF5 triode amplifier, where the feedback is applied to the galvanometer coil for comparison, and the difference between the two photocurrents is a strong function of the coil current.