## The Pauli Exclusion Principle

Contents

An electron in an atom is completely described by four quantum numbers: *n*, *l*, *m _{l}*, and

*m*. The first three quantum numbers define the orbital and the fourth quantum number describes the intrinsic electron property called spin. An Austrian physicist Wolfgang Pauli formulated a general principle that gives the last piece of information that we need to understand the general behavior of electrons in atoms.

_{s}The **Pauli exclusion principle** can be formulated as follows: No two electrons in the same atom can have exactly the same set of all the four quantum numbers. What this means is that electrons can share the same orbital (the same set of the quantum numbers *n*, *l*, and *m _{l}*), but only if their spin quantum numbers

*m*have different values. Since the spin quantum number can only have two values ),\(\left(±\phantom{\rule{0.2em}{0ex}}\frac{1}{2}\phantom{\rule{0.2em}{0ex}}\right),\) no more than two electrons can occupy the same orbital (and if two electrons are located in the same orbital, they must have opposite spins). Therefore, any atomic orbital can be populated by only zero, one, or two electrons.

_{s}The properties and meaning of the quantum numbers of electrons in atoms are briefly summarized in the table below.

## Quantum Numbers, Their Properties, and Significance | |||
---|---|---|---|

Name | Symbol | Allowed values | Physical meaning |

principal quantum number | n | 1, 2, 3, 4, …. | shell, the general region for the value of energy for an electron on the orbital |

angular momentum or azimuthal quantum number | l | 0 ≤ l ≤ n – 1 | subshell, the shape of the orbital |

magnetic quantum number | m_{l} | – l ≤ m ≤ _{l}l | orientation of the orbital |

spin quantum number | m_{s} | \(\phantom{\rule{0.2em}{0ex}}\frac{1}{2}\phantom{\rule{0.2em}{0ex}},\phantom{\rule{0.2em}{0ex}}-\frac{1}{2}\) | direction of the intrinsic quantum “spinning” of the electron |

## Example: Working with Shells and Subshells

Indicate the number of subshells, the number of orbitals in each subshell, and the values of *l* and *m _{l}* for the orbitals in the

*n*= 4 shell of an atom.

### Solution

For *n* = 4, *l* can have values of 0, 1, 2, and 3. Thus, *s*, *p*, *d*, and *f* subshells are found in the *n* = 4 shell of an atom. For *l* = 0 (the *s* subshell), *m _{l}* can only be 0. Thus, there is only one 4

*s*orbital. For

*l*= 1 (

*p*-type orbitals),

*m*can have values of –1, 0, +1, so we find three 4

*p*orbitals. For

*l*= 2 (

*d*-type orbitals),

*m*can have values of –2, –1, 0, +1, +2, so we have five 4

_{l}*d*orbitals. When

*l*= 3 (

*f*-type orbitals),

*m*can have values of –3, –2, –1, 0, +1, +2, +3, and we can have seven 4

_{l}*f*orbitals. Thus, we find a total of 16 orbitals in the

*n*= 4 shell of an atom.

## Example: Maximum Number of Electrons

Calculate the maximum number of electrons that can occupy a shell with (a) *n* = 2, (b) *n* = 5, and (c) *n* as a variable. Note you are only looking at the orbitals with the specified *n* value, not those at lower energies.

### Solution

(a) When *n* = 2, there are four orbitals (a single 2*s* orbital, and three orbitals labeled 2*p*). These four orbitals can contain eight electrons.

(b) When *n* = 5, there are five subshells of orbitals that we need to sum:

\(\begin{array}{l} \;1 \text{ orbital labeled } 5s \\ \;3 \text{ orbitals labeled } 5p \\ \;5 \text{ orbitals labeled } 5d \\ \;7 \text{ orbitals labeled } 5f \\ +9 \text{ orbitals labeled } 5g \\ \hline \;25 \text{ orbitals total }\end{array}\)

Again, each orbital holds two electrons, so 50 electrons can fit in this shell.

(c) The number of orbitals in any shell *n* will equal *n*^{2}_{.} There can be up to two electrons in each orbital, so the maximum number of electrons will be 2 \(×\) n^{2}

## Example: Working with Quantum Numbers

Complete the following table for atomic orbitals:

Orbital | n | l | m degeneracy_{l} | Radial nodes (no.) |
---|---|---|---|---|

4f | ||||

4 | 1 | |||

7 | 7 | 3 | ||

5d |

### Solution

The table can be completed using the following rules:

- The orbital designation is
*nl*, where*l*= 0, 1, 2, 3, 4, 5, … is mapped to the letter sequence s,*p*,*d*,*f*,*g*,*h*, …, - The
*m*degeneracy is the number of orbitals within an_{l}*l*subshell, and so is 2*l*+ 1 (there is one*s*orbital, three*p*orbitals, five*d*orbitals, seven*f*orbitals, and so forth). - The number of radial nodes is equal to
*n –**l*– 1.

Orbital | n | l | m degeneracy_{l} | Radial nodes (no.) |
---|---|---|---|---|

4f | 4 | 3 | 7 | 0 |

4p | 4 | 1 | 3 | 2 |

7f | 7 | 3 | 7 | 3 |

5d | 5 | 2 | 5 | 2 |