I'm afraid this question is going to sound rather dumb but here it is:

Suppose I have a very simple circuit: one battery and one resistor. The sum of the voltages in this circuit has to equal zero. My question is, how does the resistor "know" how much voltage drop to provide? How is it that it always manages accommodate a voltage drop that exactly equals to voltage provided by the battery?

Because of V=IR, I can see that if the resistance is kept constant then the current flowing across the resistor will increase or decrease according to the voltage drop needed. But how and why does this "accommodation" occur?

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    $\begingroup$ Perhaps you are simply using it as a shorthand but asking how things "know" almost always clouds the issue and keeps you from seeing how it happens. Instead ask what regulates the process. $\endgroup$ Commented Sep 27, 2014 at 17:59

2 Answers 2


The answer is simple, the resistor doesn't know what voltage drop to provide, and to some extent it doesn't "care" either (unless it's so high that the current fries it but that's another issue).

The "voltage drop" is only governed by the potential difference created by the generator (battery or other). If the circuit is open, the electrons have no path so there is no flow. As soon as the circuit is closed, the electrons have a path and start to flow across the conductor (a resistor is also a conductor).

The only thing the resistor will govern, is how strong the flow of electron will be from A to B (from one potential to another, but remember this potential was created by the generator, the resistor doesn't need to know it).

I often do the analogy between electricity and hydraulic flow. Consider the difference of potential (the voltage) created by the generator as a height, and the resistor as a slope. The flow of water will be different in the same way as the electrons in a circuit.

Consider the 3 scenario in the following image: resistors

  • Scenario A: No resistor to close the circuit => no current flow possible.
  • Scenario B: Low resistor. The electrons (or the water) fall from the high potential to the low one (rather rapidly).
  • Scenario C: The electrons (or the water) fall from high to low potential, still from the same height (your Voltage drop is identical). Except this time the higher resistance (flatter slope) makes it harder to reach the low potential (=> lower current).

Now imagine the high potential is 24V, or even 10,000, the mechanics are still the same, the electrons will flow from one potential to another as soon as they have a path, regardless of the resistor value. The only difference made by the resistor is how strong they will flow (how strong the current will be).

note: The analogies with the water flow are easily arguable and quickly reach their limits with complex circuits, this is not the exercise here. They still are a great way to explain electric current in the simple cases


It's not a dumb question.

The electrons at the negative side of the battery have energy, and will look for "any path" to get rid of that energy - move in the direction of an electric field. When you create a circuit, you move the potential of the positive terminal closer to the negative terminal. If you assume that "wire" has no resistance (for simplicity) and the only resistive element is the resistor, then the electric field (potential) along the wire must be zero, so the entire potential of the battery ends up across the resistor.

At this point, electrons say "hey, we can start to move across this resistor", and they start moving. But as they move, they experience resistance - basically they are knocked off their path from A to B, and keep having to accelerate again. This "being knocked off course" is experienced as resistance (which results in heating of the resistor) and the time it takes the electron to pick up speed again (and be knocked off course again) is a function of the electric field - the potential difference.

Thus, there is a feedback mechanism; and it turns out that "resistance" is a convenient quantity with which to describe this "losing energy" as the electron traverses the resistor. So the "accommodation" you are asking about is really happening at the microscopic level.

Does that make it clearer for you?

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    $\begingroup$ Hmm I'm not sure I understand how this solves the "accommodation" problem...The potential difference is not only a function of the electric field, it's also a function of the length of the resistor. So how and why is it that the electric field morphs to a certain value such that it matches with the specific amount of potential difference imposed by the battery? Also, you're answer stimulated another question... Because ideal conductors have no voltage drop, then they can't conduce current? As in , resistivity=E/J? $\endgroup$
    – DLV
    Commented Sep 27, 2014 at 18:09
  • $\begingroup$ @David Electric field and potential are related by the line integral $\Delta V = \int_s \, \vec{E}\cdot \mathrm{d}\vec{s}$ (or $\Delta V = E \Delta s \cos\theta$ for my algebra/trig students). The potential across the resistor follow from the battery and the properties of conduction charge on conductors, so the field will find the right configuration. $\endgroup$ Commented Sep 27, 2014 at 18:19
  • $\begingroup$ If you accept that the entire potential of the battery ends up across the resistor, then it follows that the local electric field is given by the battery voltage divided by the size of the resistor. A good microscopic description can be found at hyperphysics.phy-astr.gsu.edu/hbase/electric/ohmmic.html which may make things clearer. Note that the velocity of electrons "in random directions" is many orders of magnitude greater than the drift velocity in metals - $10^6 m/s$ vs $mm/s$. $\endgroup$
    – Floris
    Commented Sep 27, 2014 at 18:22
  • $\begingroup$ Looks like you want to know why a voltage source - for example a battery - is able to provide a constant voltage drop. Take a simpler example - a charged capacitor - and connect it to two wires. The potential between the ends of the wires will stay constant independent of the distance between those ends. In other words, the field between the wires always morphs such that the potential difference stays the same. No resistor is needed for that at all. $\endgroup$
    – Tesseract
    Commented Sep 28, 2014 at 2:29

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