Let's drop back to Ohm's Law: V = i/r, which can be rearranged as i = V/r or r = V/i, where V is volts, i is current in amps and r = Ohms.
In the circuit below, we have a battery, (which we will assume has a constant voltage regardless of load and no internal resistance), a resistor representing the circuit load and another resistor representing the resistance of the wiring and connections. The current, shown by the red line, is constant throughout the circuit, since everything is in series.
Let's say the battery provides 12 volts, the load has a resistance of 10 Ohms, and assume the wiring has 0 ohms resistance,
Use Ohm's law to find the current:
i = V/r = 12/10 = 1.2 amps.
View attachment 129812
If the cable resistance truly is zero Ohms, the voltage across the Load will be the same as the (ideal) battery voltage.
But let's say the voltage across the load only measures 11 volts. That means 1 volt is being dropped across the cable resistance, which is actually spread out rather than being a single lump like I've shown here. Back to Ohm's law. We can calculate the resistance in the cable.
We already know 1 volt is dropped across the cable resistance. But what's the current? The load is 10 Ohms we know, and there's 11 volts across it.
i = V/r = 11/10 = 1.1 amps.
The same current is flowing through the cable, so we know the voltage drop caused by the cable resistance, and the current, so
r = V/i = 1/1.1 = 0.91 Ohms = cable resistance.
Let's doublecheck our calulations.
R
load = 10 Ohms
R
cable = 0.91 Ohms
R
total = R
load + R
cable = 10 + 0.91 = 10.91 Ohms
i = V/r = 12/10.91 = 1.1 amps.