Faraday's laws of electrolysis
Pass a current through molten copper sulphate and copper metal plates out onto the cathode, atom by atom, in exact proportion to the charge you send through. That precision is not an accident — it is the content of Faraday's two laws of electrolysis, discovered by Michael Faraday in the 1830s, decades before anyone knew an electron existed. The first law says the mass deposited is directly proportional to the charge passed. The second law says that when the same charge passes through several different electrolytes in series, the masses liberated are proportional to each substance's chemical equivalent weight. Together they turn electrolysis from a qualitative curiosity into arithmetic: given a current, a time, and a formula, you can predict to the milligram how much metal will appear on an electrode. This article states both laws, connects them through the Faraday constant , and works through the coulometry calculations you need for the Electrochemistry unit.
The mass of substance deposited or liberated at an electrode is proportional to the charge passed, , and for a fixed charge the masses of different substances liberated in series are proportional to their equivalent weights, , because depositing one gram-equivalent of anything always costs exactly one Faraday of charge.
The core idea
Faraday's First Law. The mass of a substance deposited or liberated at an electrode during electrolysis is directly proportional to the quantity of electric charge passed through the electrolyte.
where: is the mass deposited or liberated (g), is the charge passed (C), is the current (A), is the time (s), and is the electrochemical equivalent — the mass deposited per coulomb of charge, a constant specific to each substance.
Faraday's Second Law. When the same quantity of charge is passed through different electrolytes connected in series, the masses of the different substances liberated at their respective electrodes are directly proportional to their chemical equivalent weights.
where: are the masses deposited in the two cells and are the equivalent weights (equivalent mass) of the two substances, .
The Faraday constant. One mole of electrons carries a charge of one Faraday, (from the more precise ). Depositing one gram-equivalent of any substance — whatever it is — always requires exactly of charge. This is the bridge between the two laws: the electrochemical equivalent and the equivalent weight are related by
so is not a random per-substance number but simply scaled by the universal constant . That single relation is why the first law (mass proportional to charge, for one substance) and the second law (mass ratios equal equivalent-weight ratios, across substances) are really the same physics seen two ways.
Linking to atomic charge. Since a mole of electrons () carries the Faraday, and each electron carries charge :
Check: . This relation lets you move between the macroscopic Faraday constant and the microscopic electronic charge without needing the details of how was first measured (the Millikan oil-drop experiment is not required at this level — only the relation itself).
The goal is to combine Faraday's First Law with the constant into a single working formula, , that turns a current-and-time problem into a mass answer in three short steps, and to show why the equivalent weight — not the molar mass — is the quantity that belongs in it.
Step 1. Start from the definition of the electrochemical equivalent. Faraday's First Law states , where is the mass deposited per coulomb. This constant is awkward to look up for every substance, so it is more useful to express it through the Faraday constant.
Step 2. Substitute . Because one gram-equivalent of any substance is deposited by exactly one Faraday of charge, the electrochemical equivalent must be the equivalent weight divided by that same charge: . Putting this into gives
Step 3. Identify what each symbol needs to be, in the right units, before you plug in numbers. must be the equivalent weight (molar mass divided by the number of electrons transferred per ion, obtained from the half-reaction such as ), must be in coulombs (current in amperes times time in seconds, not minutes or hours), and . Using molar mass in place of is the single most common error, because it silently drops the factor of the ion's charge.
Step 4. Read off the result. is the working equation for every "current, time, mass" problem in this topic — it applies equally to a metal being deposited at a cathode or a gas like or being liberated at an electrode, as long as is that species' equivalent weight for the relevant half-reaction.
Worked example
Problem. A current of is passed through molten for minutes. Calculate the mass of copper deposited at the cathode, and then find the mass of aluminium that the same charge would deposit from molten connected in series. (Molar mass of Cu , ; molar mass of Al , .)
Step 1. Charge passed: . Time was converted to seconds first, since only gives coulombs when is in seconds.
Step 2. Equivalent weight of copper: two electrons are transferred per ion, so .
Step 3. Mass of copper: .
Step 4. Equivalent weight of aluminium: three electrons are transferred per ion, so .
Step 5. Apply Faraday's Second Law directly, since the same passes through both cells in series: .
Both answers check by direct calculation too: . Final answer: and — aluminium deposits far less mass for the same charge because each mole of Al needs three electrons, spreading the same charge over a smaller equivalent weight.
Common traps
- Using molar mass instead of equivalent weight in or — always divide molar mass by the number of electrons transferred per ion to get .
- Forgetting to convert time to seconds before computing — minutes or hours left unconverted give a charge, and hence a mass, off by a large factor.
- Applying Faraday's Second Law to cells that are not connected in series — the equal-charge condition needed for only holds automatically in a series circuit.
- Treating (electrochemical equivalent) as one fixed number for all substances — it equals and is different for every ion, so it must be recalculated each time.
Ask the tutor: Want to try a Faraday's-laws numerical with a gas liberated at an electrode instead of a metal deposited, or see how the equivalent weight changes for an ion with a different charge?
Why does the same charge deposit different masses of copper and aluminium?
Because charge is shared per electron transferred, not per atom. Depositing one copper atom needs two electrons (), while depositing one aluminium atom needs three (). For the same charge, fewer electrons per atom means more atoms — and hence more mass — can be deposited. That is exactly what the equivalent weight captures, which is why Faraday's Second Law compares equivalent weights rather than molar masses.
Do I need to remember the exact value of the Faraday constant, or can I derive it?
For numericals you should use directly — it is a standard given value. But you should also know and be able to reproduce the relation , since one mole of electrons () each carrying charge multiplies out to , matching within rounding. You are not expected to know how itself was measured experimentally (that belongs to the Millikan oil-drop experiment, outside this syllabus) — only this algebraic relation between , and .
Is Faraday's Second Law just a restatement of the first, or genuinely new information?
It is genuinely new, but the two are unified by one idea: one gram-equivalent of anything costs exactly one Faraday. The First Law tells you how mass scales with charge for a single substance: double the charge, double the mass. The Second Law tells you how to compare two different substances when the same charge passes through both — something the First Law alone cannot do, since it says nothing about a second substance's electrochemical equivalent. Once you know , however, both laws collapse into the single working equation , applied once for each cell.