Title: The world of Atoms
1The world of Atoms
2Quantum Mechanics
Theory that describes the physical properties of
smallest particles (atoms, protons, electrons,
photons)
3The hydrogen atom
- electron orbits around the nucleus like a wave
- orbit is described by wavefunction
- wavefunction is discrete solution of wave
equation
- only certain orbits are allowed
- orbits correspond to energy levels of atom
4The hydrogen atom
In the Bohr model of the atom, the hydrogen atom
is like a planetary system with the electron in
certain allowed circular orbits.
The Bohr model does not work for more complicated
systems!
5Quantum numbers
Each orbital is characterized by a set of quantum
numbers.
Principal quantum number (n) integral values
(1,2,3). Related to the size and energy of the
orbital.
Angular momentum quantum number (l) integral
values from 0 to (n-1) for each value of n.
Magnetic quantum number (ml) integral values
from - l to l for each value of n.
6Quantum numbers
How many orbitals are there for each principle
quantum number n 2 and n 3?
For each n, there are n different l-levels and
(2l1) different ml levels for each l.
n2
n 2
different l-levels
l 0, 1
(2l1) 2 x 0 1
1 ml-levels for l 0
(2l1) 2 x 1 1
3 ml-levels for l 1
Total 1 3 4 levels
for n 2
7Quantum numbers
How many orbitals are there for each principle
quantum number n 2 and n 3?
For each n, there are n different l-levels and
(2l1) different ml levels for each l.
n3
n 3
different l-levels
l 0, 1,2
(2l1) 2 x 0 1
1 ml-levels for l 0
(2l1) 2 x 1 1
3 ml-levels for l 1
(2l1) 2 x 2 1
5 ml-levels for l 2
Total 1 3 5 9 levels for n 3
The total number of levels for each n is n2
8Quantum numbers
Names of atomic orbitals are derived from value
of l
9Quantum numbers
Quantum numbers for the first four levels in the
hydrogen atom.
10What is the meaning of ?
Wavefunction itself is not an observable!
Square of wavefunction is proportional to
probability density
11Wavefunction and probability
12Quantum numbers
A subshell is a set of orbitals with the same
value of l. They have a number for n and a
letter indicating the value of l.
l 0 (s)
l 1 (p)
l 2 (d)
l 3 (f)
l 4 (g)
13Orbital Shapes
14Heisenberg uncertainty principle
15Heisenberg uncertainty principle
It is not possible to know both the position and
momentum of an electron at the same time with
infinite precision.
16Heisenberg
17The s orbitals in hydrogen
probability distributions
The higher energy orbitals have nodes, or regions
of zero electron density.
s-orbitals have n-1 nodes.
The 1s orbital is the ground state for hydrogen.
orbital surfaces
18Pauli exclusion principle
How many electrons fit into 1 orbital?
Only 2 electrons fit into 1 orbital
1 spin up
1 spin down
19Pauli exclusion principle
Electrons are fermions. There are also bosons
As the temperature is lowered, bosons pack much
closer together, while fermions remain spread
out.
20Energy Levels
21Energy Transitions
For the energy change when moving from one level
to another
22Lines and Colors
Change in energy corresponds to a photon of a
certain wavelength
23Lines and Colors
What is the wavelength of the photon that is
emitted when the hydrogen atom falls from n3
into n2?
24Light out of Molecules
hydrogen
Fluorescence
25Degeneracy
Orbital energy levels for the hydrogen atom.
26Beyond hydrogen
Hydrogen is the simplest element of the periodic
table.
Exact solutions to the wave equations for other
elements do not exist!
27Polyelectric Atoms
What do the orbitals of non-hydrogen atoms look
like?
Multiple electrons electron correlation
Due to electron correlation, the orbitals in
non-hydrogen atoms have slightly different
energies
28Polyelectric Atoms
Screening due to electron repulsion, electrons
in different orbits feel a different attractive
force from the nucleus
11
Screening changes the energy of the electron
orbital the electron is less tightly bound.
29Polyelectric Atoms
Penetration within a subshell (n), the orbital
with the lower quantum number l will have higher
probability closer to the nucleus
30Polyelectric Atoms
Hydrogen
Polyelectric atom
Orbitals with the same quantum number n are
degenerate
Degeneracy is gone Ens lt Enp lt End lt Enf
31Spectra of Polyelectric Atoms
Due to lifting of degeneracy, many more lines are
possible in the spectra of polyelectric atoms