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 F=NAeF = N_Ae, and works through the coulometry calculations you need for the Electrochemistry unit.

The core insight

The mass of substance deposited or liberated at an electrode is proportional to the charge passed, w=ZQw = ZQ, and for a fixed charge the masses of different substances liberated in series are proportional to their equivalent weights, w1/w2=E1/E2w_1/w_2 = E_1/E_2, 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.

w∝Q  ⟹  w=ZQ=Zitw \propto Q \implies w = ZQ = Zit

where: ww is the mass deposited or liberated (g), Q=itQ = it is the charge passed (C), ii is the current (A), tt is the time (s), and ZZ 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.

w1w2=E1E2\frac{w_1}{w_2} = \frac{E_1}{E_2}

where: w1,w2w_1, w_2 are the masses deposited in the two cells and E1,E2E_1, E_2 are the equivalent weights (equivalent mass) of the two substances, E=molar massnumber of electrons transferred per ionE = \dfrac{\text{molar mass}}{\text{number of electrons transferred per ion}}.

The Faraday constant. One mole of electrons carries a charge of one Faraday, F=96,500 C mol−1F = 96{,}500\ \text{C mol}^{-1} (from the more precise 96,485 C mol−196{,}485\ \text{C mol}^{-1}). Depositing one gram-equivalent of any substance — whatever it is — always requires exactly 1 F1\ F of charge. This is the bridge between the two laws: the electrochemical equivalent and the equivalent weight are related by

Z=EFZ = \frac{E}{F}

so ZZ is not a random per-substance number but simply EE scaled by the universal constant FF. 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 FF to atomic charge. Since a mole of electrons (NA=6.022×1023N_A = 6.022\times10^{23}) carries the Faraday, and each electron carries charge e=1.602×10−19 Ce = 1.602\times10^{-19}\ \text{C}:

F=NA eF = N_A\, e

Check: 6.022×1023×1.602×10−19=96,472 C mol−1≈96,500 C mol−16.022\times10^{23} \times 1.602\times10^{-19} = 96{,}472\ \text{C mol}^{-1} \approx 96{,}500\ \text{C mol}^{-1}. This relation lets you move between the macroscopic Faraday constant and the microscopic electronic charge without needing the details of how ee was first measured (the Millikan oil-drop experiment is not required at this level — only the relation F=NAeF = N_Ae itself).

Figure
Two electrolytic cells in series with the same current flowing through both showing copper deposited at one cathode and aluminium deposited at the other in the ratio of their equivalent weights
Same charge, two cells in series — masses follow equivalent weights battery i CuSO4 cell Cu deposits anode AlCl3 cell Al deposits anode Same Q through both — w(Cu)/w(Al) = E(Cu)/E(Al)
Derivation AMass deposited from charge, current and equivalent weight

The goal is to combine Faraday's First Law with the constant Z=E/FZ = E/F into a single working formula, w=EQ/Fw = EQ/F, 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 w=ZQw = ZQ, where ZZ 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 Z=E/FZ = E/F. 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: Z=E/FZ = E/F. Putting this into w=ZQw = ZQ gives

w=EQF=E i tFw = \frac{EQ}{F} = \frac{E \, i \, t}{F}

Step 3. Identify what each symbol needs to be, in the right units, before you plug in numbers. EE must be the equivalent weight (molar mass divided by the number of electrons transferred per ion, obtained from the half-reaction such as Cu2++2e−→Cu\text{Cu}^{2+} + 2e^- \rightarrow \text{Cu}), QQ must be in coulombs (current in amperes times time in seconds, not minutes or hours), and F=96,500 C mol−1F = 96{,}500\ \text{C mol}^{-1}. Using molar mass in place of EE is the single most common error, because it silently drops the factor of the ion's charge.

Step 4. Read off the result. w=EitFw = \dfrac{Eit}{F} 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 Cl2\text{Cl}_2 or H2\text{H}_2 being liberated at an electrode, as long as EE is that species' equivalent weight for the relevant half-reaction.

Worked example

Problem. A current of 2 A2\ \text{A} is passed through molten CuSO4\text{CuSO}_4 for 3030 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 AlCl3\text{AlCl}_3 connected in series. (Molar mass of Cu =63.5 g mol−1= 63.5\ \text{g mol}^{-1}, Cu2++2e−→Cu\text{Cu}^{2+} + 2e^- \rightarrow \text{Cu}; molar mass of Al =27 g mol−1= 27\ \text{g mol}^{-1}, Al3++3e−→Al\text{Al}^{3+} + 3e^- \rightarrow \text{Al}.)

Step 1. Charge passed: Q=it=2×(30×60)=2×1800=3600 CQ = it = 2 \times (30 \times 60) = 2 \times 1800 = 3600\ \text{C}. Time was converted to seconds first, since Q=itQ = it only gives coulombs when tt is in seconds.

Step 2. Equivalent weight of copper: two electrons are transferred per Cu2+\text{Cu}^{2+} ion, so ECu=63.5/2=31.75 g eq−1E_{\text{Cu}} = 63.5/2 = 31.75\ \text{g eq}^{-1}.

Step 3. Mass of copper: wCu=ECu QF=31.75×360096,500=114,30096,500=1.184 gw_{\text{Cu}} = \dfrac{E_{\text{Cu}} \, Q}{F} = \dfrac{31.75 \times 3600}{96{,}500} = \dfrac{114{,}300}{96{,}500} = 1.184\ \text{g}.

Step 4. Equivalent weight of aluminium: three electrons are transferred per Al3+\text{Al}^{3+} ion, so EAl=27/3=9.0 g eq−1E_{\text{Al}} = 27/3 = 9.0\ \text{g eq}^{-1}.

Step 5. Apply Faraday's Second Law directly, since the same 3600 C3600\ \text{C} passes through both cells in series: wCuwAl=ECuEAl  ⟹  wAl=wCu×EAlECu=1.184×9.031.75=1.184×0.2835=0.336 g\dfrac{w_{\text{Cu}}}{w_{\text{Al}}} = \dfrac{E_{\text{Cu}}}{E_{\text{Al}}} \implies w_{\text{Al}} = w_{\text{Cu}} \times \dfrac{E_{\text{Al}}}{E_{\text{Cu}}} = 1.184 \times \dfrac{9.0}{31.75} = 1.184 \times 0.2835 = 0.336\ \text{g}.

Both answers check by direct calculation too: wAl=EAlQ/F=(9.0×3600)/96,500=0.336 gw_{\text{Al}} = E_{\text{Al}}Q/F = (9.0 \times 3600)/96{,}500 = 0.336\ \text{g}. Final answer: wCu≈1.18 gw_{\text{Cu}} \approx 1.18\ \text{g} and wAl≈0.336 gw_{\text{Al}} \approx 0.336\ \text{g} — 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 w=ZQw = ZQ or w=Eit/Fw = Eit/F — always divide molar mass by the number of electrons transferred per ion to get EE.
  • Forgetting to convert time to seconds before computing Q=itQ = it — 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 w1/w2=E1/E2w_1/w_2 = E_1/E_2 only holds automatically in a series circuit.
  • Treating ZZ (electrochemical equivalent) as one fixed number for all substances — it equals E/FE/F 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 (Cu2++2e−→Cu\text{Cu}^{2+} + 2e^- \rightarrow \text{Cu}), while depositing one aluminium atom needs three (Al3++3e−→Al\text{Al}^{3+} + 3e^- \rightarrow \text{Al}). 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 E=molar mass/electrons transferredE = \text{molar mass}/\text{electrons transferred} 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 F=96,500 C mol−1F = 96{,}500\ \text{C mol}^{-1} directly — it is a standard given value. But you should also know and be able to reproduce the relation F=NAeF = N_Ae, since one mole of electrons (NA=6.022×1023N_A = 6.022\times10^{23}) each carrying charge e=1.602×10−19 Ce = 1.602\times10^{-19}\ \text{C} multiplies out to 96,472 C mol−196{,}472\ \text{C mol}^{-1}, matching 96,50096{,}500 within rounding. You are not expected to know how ee itself was measured experimentally (that belongs to the Millikan oil-drop experiment, outside this syllabus) — only this algebraic relation between FF, NAN_A and ee.

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 Z=E/FZ = E/F, however, both laws collapse into the single working equation w=Eit/Fw = Eit/F, applied once for each cell.

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