Faraday's laws of electrolysis
Faraday's laws of electrolysis are quantitative relationships based on the electrochemical research published by Michael Faraday in 1833.[1][2][3]
First law
Michael Faraday reported that the mass (m) of elements deposited at an electrode is directly proportional to the charge (Q; SI units are ampere seconds or coulombs).[3]
Here, the constant of proportionality, Z, is called the electro-chemical equivalent (ECE) of the substance. Thus, the ECE can be defined as the mass of the substance deposited/liberated per unit charge.
Second law
Faraday discovered that when the same amount of electric current is passed through different electrolytes/elements connected in series, the mass of the substance liberated/deposited at the electrodes is directly proportional to their chemical equivalent/equivalent weight (E).[3] This turns out to be the molar mass (M) divided by the valence (v)
Derivation
A monovalent ion requires 1 electron for discharge, a divalent ion requires 2 electrons for discharge and so on. Thus, if x electrons flow, atoms are discharged.
So the mass m discharged is
where
- NA is the Avogadro constant;
- Q = xe is the total charge, equal to the number of electrons (x) times the elementary charge e;
- F is the Faraday constant.
Mathematical form
Faraday's laws can be summarized by
where M is the molar mass of the substance (usually given in SI units of grams per mole) and v is the valency of the ions .
For Faraday's first law, M, F, v are constants; thus, the larger the value of Q, the larger m will be.
For Faraday's second law, Q, F, v are constants; thus, the larger the value of (equivalent weight), the larger m will be.
In the simple case of constant-current electrolysis, Q = It, leading to
and then to
where:
- n is the amount of substance ("number of moles") liberated:
- t is the total time the constant current was applied.
For the case of an alloy whose constituents have different valencies, we have
where wi represents the mass fraction of the i-th element.
In the more complicated case of a variable electric current, the total charge Q is the electric current I(τ) integrated over time τ:
Here t is the total electrolysis time.[4]
References
- Faraday, Michael (1834). "On Electrical Decomposition". Philosophical Transactions of the Royal Society. 124: 77–122. doi:10.1098/rstl.1834.0008. S2CID 116224057.
- Ehl, Rosemary Gene; Ihde, Aaron (1954). "Faraday's Electrochemical Laws and the Determination of Equivalent Weights". Journal of Chemical Education. 31 (May): 226–232. Bibcode:1954JChEd..31..226E. doi:10.1021/ed031p226.
- "Faraday's laws of electrolysis | chemistry". Encyclopedia Britannica. Retrieved 2020-09-01.
- For a similar treatment, see Strong, F. C. (1961). "Faraday's Laws in One Equation". Journal of Chemical Education. 38 (2): 98. Bibcode:1961JChEd..38...98S. doi:10.1021/ed038p98.
Further reading
- Serway, Moses, and Moyer, Modern Physics, third edition (2005), principles of physics.
- Experiment with Faraday's laws