Chemistry · Ch 2 — Quantum Mechanical Model of Atom
Quantum numbers
Quantum numbers
A single electron inside an atom is fully characterised by a set of four quantum numbers: the principal quantum number , the azimuthal (subsidiary) quantum number , the magnetic quantum number , and the spin quantum number . It's worth noting where each of these actually comes from mathematically: solving the Schrödinger equation for a wavefunction naturally produces the first three - , and - as the parameters needed to specify a valid solution. The fourth quantum number, spin, does not come out of that same spatial wave equation at all; it arises separately, from the fact that the electron itself spins about its own axis. (That said, picturing this literally as a tiny sphere physically spinning like a top is misleading and not to be taken as a literal classical picture - "spin" is a genuinely quantum property that simply behaves, in some ways, analogously to classical spinning.)
Principal quantum number (). This number specifies which energy shell the electron occupies - the shell it "revolves" in - and is denoted by the letter .
- can take positive integer values . Shells are also given letter names: is called the K shell, is the L shell, and are the M, N and O shells respectively.
- The maximum number of electrons a given shell can hold is .
- alone fixes both the electron's energy, kJ mol, and its average distance from the nucleus, Å - the same formulas already met in the Bohr model, now reinterpreted as quantum-mechanical results rather than as classical orbit properties.
Azimuthal (subsidiary) quantum number ().
- Denoted by the letter , it can take any integer value from up to for a given shell.
- Each distinct value of defines a subshell (equivalently, describes the shape of the orbitals in that subshell): correspond to the s, p, d, f and g subshells respectively.
- The maximum number of electrons a given subshell can hold is .
- also fixes the size of the electron's orbital angular momentum, through
Magnetic quantum number ().
- Denoted , it takes integer values running from to passing through 0 - so for example if , then .
- For a fixed , each different value of represents a different spatial orientation of that subshell's orbitals.
- The experimental evidence for this quantum number is the Zeeman effect - the splitting of spectral lines when an atom is placed in a magnetic field, which happens precisely because the different orientations, ordinarily all of equal energy, are pulled apart in energy once an external field singles out a preferred direction in space.
- To put it another way: fixes the magnitude of the orbital angular momentum, while fixes its direction.
Spin quantum number ().
- This quantum number represents the electron's own intrinsic spin and is denoted .
- Loosely, it is described as the electron spinning about its own axis either clockwise or anticlockwise - but as noted above, this literal picture is not physically accurate; spin is better understood simply as an intrinsic property that reveals itself experimentally through the electron's behaviour in a magnetic field.
- Correspondingly, only two values of this quantum number are possible, matching the two senses of "clockwise" and "anticlockwise." …
| Shell | Principal quantum number (n) | Max. electrons in shell | Azimuthal quantum number (l) | Max. electrons in a subshell | Magnetic quantum number (m) – orbital orientations | Designation of orbitals in the shell |
|---|---|---|---|---|---|---|
| K | 1 | 2 | 0 | 2 | 0 | 1s |
| L | 2 | 8 | 0 | 2 | 0 | 2s |
| L | 2 | 8 | 1 | 6 | −1, 0, +1 | |
| M | 3 | 18 | 0 | 2 | 0 | 3s |
| M | 3 | 18 | 1 | 6 | −1, 0, +1 | |
| M | 3 | 18 | 2 | 10 | −2, −1, 0, +1, +2 | |
| N | 4 | 32 | 0 | 2 | 0 | 4s |
| N | 4 | 32 | 1 | 6 | −1, 0, +1 | |
| N | 4 | 32 | 2 | 10 | −2, −1, 0, +1, +2 | |
| N | 4 | 32 | 3 | 14 | −3, −2, −1, 0, +1, +2, +3 | seven f orbitals: |