Chemistry 401

Multielectron atoms

We can not solve the Schroedinger equation exactly so assumptions must be made.

Usual assumption: the hydrogenic obitals are adequate and electrons occupy them in some fashion.

 

The occupation of electrons in orbitals is called the electron configuration – this is one way to describe the electronic properties of atoms.

 

Two guiding principals used to account for electron configurations:

Aufbau Principle: electrons occupy orbitals in such a manner to give the lowest possible total energy

Pauli Exclusion Principle: each electron in an atom is described by a unique set of quantum numbers (n, l, ml, ms) - i.e., two electrons per hydrogenic orbital

Periodic Table: based on electron configurations and can be used to predict them but not absolute (electron configurations are experimental quantities)

Aids in finding correct electron configurations from the Periodic Table:

Half-filled phenomenon: when d or f electrons are the valence shell, if a shift of 1 electron (occasionally 2 but this is not predictive) from an s orbital to the d or f orbital leads to a filled or half filled d or f orbital, this will stabilize the electron configuration.

Anions: add electrons to the neutral atom and follow above rules.

Cations: electrons are always removed from the orbitals of neutral atoms with the largest principal quantum number (n); the remaining electrons fill the orbitals with the lowest n consistent with the Pauli Principle

 

Term Symbols

Another way to indicate electron configurations

A term symbol gives the required information about the angular momentum quantum numbers l, m<l, and ms

For Ground States of atoms:

1) Only consider unfilled subshells; filled shells do not contribute

2) Fill the valence electrons into the unfilled subshell such that the highest total spin is attained using the highest possible ml values (this is Hund's Rule)

3) L = Σml

4) S = Σms

5) The term symbol is written as 2S+1L

2S+1 is called the total spin multiplicity or degeneracy and is written as a number

L is the total orbital angular momentum and is written as a letter:

Lletter designation

 

0S

 

1P

 

2D

 

3F

 

4G

 

5H

 

6I

 

Periodic Properties

 

Consider Li:

How good is such an approximation?

pretty good for s orbitals - they overlap the nucleus

mediocre for p orbitals - nodal at the nucleus

poor for d or f orbitals - multiply nodal at the nucleus

The reduction of nuclear charge seen by outer electrons due to the inner electrons is called screening or shielding

quantitatively:

Z* = Z - σ

Z* = effective nuclear charge

Z = true nuclear charge

σ = shielding constant

Shielding constants are established by ad hoc rules or quantum mechanical calculations

Trends in Z*

s orbitals are good screeners, p orbitals are moderate screeners; d, f orbitals are very poor screeners.

This means changes across the Table are bigger than changes down the Table

 

Experimental Properties

Ionization Potential (IP) or Ionization Energy (IE)

A(g) A+(g) + e

The energy associated with this reaction is the ionization energy

IP or IE is thermodynamically positive

IP generally follows Z* across the Table

 

Electron Affinity : EA

A(g) + eA(g)

EA reported with the wrong thermodynamic sign

Periodic trends are reverse of IP

Atomic Size : Radius of an atom - a difficult concept to define

atomic radius depends upon the bonding situation

metallic radius : ½ the internuclear distance between atoms in the metallic state

covalent radius : ½ the internuclear distance in a homonuclear covalent bond

ionic radius : size of an ion in a solid

van der Waals radius : the distance at which an atom just starts to respond to interactions from neighboring atoms

radii all of different numerical values but similar periodic trends:

r increases as go down the Periodic Table (bigger n)

r decreases as go across the Periodic Table (bigger Z*)