Lets examine this circuit/system, which has a SignalGround of length 13 feet, running from the 100 microvolt Return wire of the Moving Coil vinyl record playback cartridge, thru 5' coax, thru RIAA preamp, thru 3' of coax to the 100 watt Audio Power Amplifier, then thru 5' of Speaker Return wire to the speaker (which has about 100 volts PeakPeak, or 1,000,000X larger than the sensor signal).

simulate this circuit – Schematic created using CircuitLab
Signal Ground runs all the way from the MovingCoil sensor which is left-most 1uH inductor (bottom node of that inductor is the "ground") thru the 5 feet of cable to the J1 JFET, to the RIAA capacitors (C3 and C4), thru the rest of the low-noise RIAA preamplifier transistors, out the COAX CABLE to the 100 watt audio power amplifier, and finally to ONE of the leads to the speaker.
The non-ground wire of the speaker will have substantial signal voltage {100 watts and 8 ohms => ~ 30 volts RMS or 100 volts PeakPeak), and electric fields will couple to EARTH, with those currents needing to find a path back home.
The designer gets to DESIGN all these paths. Its an incremental process of learning. For now, start with viewing a sheet of copper as your ground.
The (charging, or displacement) current thru a capacitor is I = C * dV/dt.
The dV/dT of 100 volts at 60Hz is 100 * (60 * 2 * pi) = 100 * 377 = 37,700 volts per second.
Now we need the "capacitance".
What is the capacitance between you and the earth thru your shoes?
What is the capacitance between two wires? look up the wire-wire capacitance formul (Electric Fields between two wires)
What is the capacitance between a wire and a plate?
After you ask these questions, and you gather up just a few (4? 5?) formulas, you can perform your own analysis of electric-field-induced stray currents. You will begin to think about shielding, and you will be on the way to designing high-fidelity (high signal-noise-ratio) circuits and systems.