Title: Chapter 7 Atomic Energies and Periodicity
1Chapter 7Atomic Energies and Periodicity
- Department of Chemistry and Biochemistry
- Seton Hall University
2Nuclear Charge
- n - influences orbital energy
- Z - nuclear charge also has a large effect
- We can measure this by ionization energies (IE)
- A ? A e-
- Consider H and He
- H ? H e- 2.18 ? 10-18 J
- He ? He e- 8.72 ? 10-18 J
- Orbital stability increases with Z2
3Electron-electron Repulsion
- Negatively charged electron is attracted to the
positively charged nucleus but repelled by
negatively charged electrons - Screening, ?, is a measure of the extent to which
some of the attraction of an electron to the
nucleus is cancelled out by the other electrons - Effective nuclear charge
- Zeff Z - ?
4Screening
- Complete screening would mean that each electron
would experience a charge of 1 - Consider He
- w/o screening the IE would be the same as for He
- Complete screening the IE would be the same as
for H - Actual IE is between the two values
5Screening
- Screening is incomplete because both electrons
occupy an extended region of space, so neither is
completely effective at screening the other from
the He2 nucleus - Compact orbitals (low values of n) are more
effective as screening since they are packed
tightly around the nucleus - Therefore, ? decreases with orbital size (as n
increases)
6Screening
- Electrons in orbitals of a given value n screen
the electrons in orbitals with larger values of n - Screening also depends on orbital shape (electron
density plots, ?2 vs r, help show this) - Generally, the larger the value of l, the more
that orbital is screened by smaller, more compact
orbitals - Quantitative information about this can be
obtained from photoelectron spectroscopy
7Structure of the periodic table
- The periodic table is arranged the way it is
because the properties of the elements follow
periodic trends - Elements in the same column have similar
properties - Elemental properties change across a row (period)
8Electron configurations
- The Pauli Exclusion Principle
- No two electrons can have the same four quantum
numbers - Hunds rule
- The most stable configuration is the one with the
most unpaired electrons - The aufbau principle
- each successive electron is placed in the most
stable orbital whose quantum numbers are not
already assigned to another electron
9Orbital diagrams and rules
- The Pauli Exclusion Principle - no two electrons
may have the same four quantum numbers. - Practically, if two electrons are in the same
orbital, they have opposite spins - Hunds Rule - when filling a subshell, electrons
will avoid entering an orbital that already has
an electronic in it until there is no other
alternative - Consider the dorm room analogy (I suggested this
to the author!!!)
10Summary of the rules
- Each electron in an atom occupies the most stable
orbital available - No two electrons can have the same four quantum
numbers - The higher the value of n, the less stable the
orbital - For equal values of n, the higher value of l, the
less stable the orbital
11Shell designation
- The shell is indicated by the principle quantum
number n - The subshell is indicated by the letter
appropriate to the value of l - The number of electrons in the subshell is
indicated by a right superscript - For example, 4p3
12Electronic configurations
- We use only as many subshells and shells as are
needed for the number of electrons - The number of available subshells depends on the
shell that is being filled - n 1 only has an s subshell
- n 2 has s and p subshells
- n 3 has s, p and d subshells
13Example
- Consider S
- Sulfur has 16 electrons
- Electronic configuration is therefore1s22s22p63s2
3p4 - d and f subshells are used for heavier elements
- You are expected to do this for any element up to
Ar
14Core and valence shells
- Chemically, we find that the electrons in the
shell with the highest value of n are the ones
involved in chemical reactions - This shell is termed the valence shell
- Electrons in shells with lower n values are
chemically unreactive because they are of such
low energy. - These shells are grouped together as the core
15Electron configurations and the periodic table
- We develop a shorthand for the electron
configuration by noting that the core is really
the same as the electron configuration for the
noble gas that occurs earlier in the periodic
table - E.g. for S (1s22s22p63s23p4), the core is
1s22s22p6 which is the same as the electron
configuration for Ne
16Atomic properties
- Ionization energy (IE)A(g) ? A(g) e-
- Electron affinity (EA)A(g) e- ? A-(g)
- Ion sizes
- Cations are smaller than the neutral atom
- Anions are larger that the neutral atom
17Electron configuration shorthand
- We can then write the electron configuration of S
as Ne3s23p4 - We note that the valence shell electron
configuration has the same pattern for elements
in the same group - For S (a chalcogen) all the elements have the
valence electron configurationcorens2np4
18Periodic trends
- Atomic radii decrease across a period
- Atomic radii increase down a group
- Ionization energies increase across a period
- Ionization energies decrease down a group
19Near degenerate orbitals
- degenerate orbitals are those that have the same
energy - normally, certain orbitals will be degenerate for
quantum mechanical reasons - near degenerate orbitals have close to the same
energy for a variety of reasons
20Ion electronic configurations
- Electronic configurations for ions involves
adding or subtracting electrons from the
appropriate atomic configuration - Example Na ? Na
- 1s22s22p63s1 ? 1s22s22p6
- Example Cl ? Cl-
- 1s22s22p63s23p5 ? 1s22s22p63s23p6
21Magnetic properties
- The spin of electrons generates a magnetic field
- Two types of magnetism
- Diamagnetism - all electrons are paired
- Paramagnetism - one or more electrons are
unpaired - In solids, two types of condensed phase magnetism
results in bulk magnetic properties -
ferromagnetism and antiferromagnetism
22Energetics of ionic compounds
- Ions in solids have very strong attractions
(ionic bonding) - Due mostly to cation-anion attraction, and
includes a component termed lattice energy - We can calculate this energy from a Born Haber
cycle
23Path yielding a net reaction
- Vaporization ?Evaporization 108 kJ/mol
- Ionization ?E IE 495.5 kJ/mol
- Bond breakage ?E Β½(bond energy) 120 kJ/mol
- Ionization ?E EA -348.5 kJ/mol
- Condensation - includes all ion-ion attractive
and repulsive interactions (the lattice energy)
24The Born-Haber Cycle
25Calculating the lattice energy
- Coulombs law allows us to calculate the
electrical force between charged particles - q1,q2 are the electrical charges of the particles
- k 1.389 ? 105 kJ pm/mol
- r interionic distance in pm
26Calculating the lattice energy
- Result of calculation yields a value of -444
kJ/mol - This includes only part of the lattice energy,
since the coulombic interactions do not stop at
the individual ions pairs. - An expansion of Coulombs law to include the
three dimensional ion interactions yields a value
for the lattice energy of -781 kJ/mol
273 D interaction in crystal
- Note that NaCl extends in all directions
- Each ion experiences attractions and repulsions
from other ions past the ones directly in contact
28The overall ionic bonding energy
- The energy for the overall processNa(s) Β½Cl2
(g) ? NaCl(s) - Calculated -406 kJ/mol
- Actual -411 kJ/mol
- This treatment assumes the interaction between
Na and Cl- is only ionic. The slight
discrepancy is ascribed to a small degree of
electron sharing
29Why not Na2Cl2-?
- Main reason is the very large ionization energy
of the core of NaNa ? Na IE1 495.5
kJ/molNa ? Na2 IE2 4562 kJ/mol - EA2 for Cl is expected to be large and positive
- Basic point is that it costs way too much energy
to ionize the core of Na
30Ion stability
- Group 1 and 2 ions will lose all of their valence
electrons - Above Group 2, removal of all valence electrons
is generally not observed - Anions will generally add enough valence
electrons to fill the valence shell