Title: Chapter 6 Electronic Structure of Atoms
1Chapter 6Electronic Structure of Atoms
2Electronic Structure
- Our goal
- Understand why some substances behave as they do.
- For example Why are K and Na reactive metals?
Why do H and Cl combine to make HCl? Why are
some compounds molecular rather than ionic? - Atom interact through their outer parts, their
electrons. - The arrangement of electrons in atoms are
referred to as their electronic structure. - Electron structure relates to
- Number of electrons an atom possess.
- Where they are located.
- What energies they possess.
3The Wave Nature of Light
- Study of light emitted or absorbed by substances
has lead to the understanding of the electronic
structure of atoms. - Characteristics of light
- All waves have a characteristic wavelength, l,
and amplitude, A. - The frequency, n, of a wave is the number of
cycles which pass a point in one second. - The speed of a wave, v, is given by its frequency
multiplied by its wavelength - For light, speed c.
4Identifying ? and ?
5Electromagnetic Radiation
- Modern atomic theory arose out of studies of the
interaction of radiation with matter. - Electromagnetic radiation moves through a vacuum
with a speed of 2.99792458 ? 10-8 m/s. - Electromagnetic waves have characteristic
wavelengths and frequencies. - Example visible radiation has wavelengths
between 400 nm (violet) and 750 nm (red).
6The Electromagnetic Spectrum
7Class Guided Practice Problem
- The yellow light given off by a sodium vapor lamp
used for public lighting has a wavelength of 589
nm. What is the frequency of this radiation?
Class Practice Problem
- A laser used to weld detached retinas produces
radiation with a frequency of 4.69 x 1014 s-1.
What is the wavelength of this radiation?
8Quantized Energy and Photons
- Planck energy can only be absorbed or released
from atoms in certain amounts chunks called
quanta. - The relationship between energy and frequency is
- where h is Plancks constant (6.626 ? 10-34 J.s).
- To understand quantization consider walking up a
ramp versus walking up stairs - For the ramp, there is a continuous change in
height whereas up stairs there is a quantized
change in height.
9The Photoelectric Effect
- Plancks theory revolutionized experimental
observations. - Einstein
- Used plancks theory to explain the photoelectric
effect. - Assumed that light traveled in energy packets
called photons. - The energy of one photon
10Class Guided Practice Problem
- Calculate the energy of a photon of yellow light
whose wavelength is 589 nm.
Class Practice Problem
- (a)Calculate the smallest increment of energy (a
quantum) that can be emitted or absorbed at a
wavelength of 803 nm. (b) Calculate the energy
of a photon of frequency 7.9 x 1014 s-1. (c) What
frequency of radiation has photons of energy 1.88
x 10-18 J? Now calculate the wavelength.
11Line Spectra and the Bohr Model
- Line Spectra
- Radiation composed of only one wavelength is
called monochromatic. - Most common radiation sources that produce
radiation containing many different wavelengths
components, a spectrum. - This rainbow of colors, containing light of all
wavelengths, is called a continuous spectrum. - Note that there are no dark spots on the
continuous spectrum that would correspond to
different lines.
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13Specific Wavelength Line Spectra
When gases are placed under reduced pressure in a
tube and a high voltage is applied, radiation at
different wavelengths (colors) will be emitted.
14Line Spectra
- Balmer discovered that the lines in the visible
line spectrum of hydrogen fit a simple equation. - Later Rydberg generalized Balmers equation to
-
- where RH is the Rydberg constant (1.096776 ? 107
m-1), h is Plancks constant (6.626 ? 10-34 Js),
n1 and n2 are integers (n2 gt n1).
15Bohr Model
- Rutherford assumed the electrons orbited the
nucleus analogous to planets around the sun. - However, a charged particle moving in a circular
path should lose energy. - This means that the atom should be unstable
according to Rutherfords theory. - Bohr noted the line spectra of certain elements
and assumed the electrons were confined to
specific energy states. These were called orbits.
16Line Spectra (Colors)
- Colors from excited gases arise because electrons
move between energy states in the atom.
17Line Spectra (Energy)
- Since the energy states are quantized, the light
emitted from excited atoms must be quantized and
appear as line spectra. - After lots of math, Bohr showed that
- where n is the principal quantum number (i.e., n
1, 2, 3, and nothing else).
18Limitations of the Bohr Model
- Can only explain the line spectrum of hydrogen
adequately. - Electrons are not completely described as small
particles.
19The Wave Behavior of Matter
- Knowing that light has a particle nature, it
seems reasonable to ask if matter has a wave
nature. - Using Einsteins and Plancks equations, de
Broglie showed - The momentum, mv, is a particle property, whereas
? is a wave property. - de Broglie summarized the concepts of waves and
particles, with noticeable effects if the objects
are small.
20The Wave Behavior of Matter
- The Uncertainty Principle
- Heisenbergs Uncertainty Principle on the mass
scale of atomic particles, we cannot determine
exactly the position, direction of motion, and
speed simultaneously. - For electrons we cannot determine their momentum
and position simultaneously. - If Dx is the uncertainty in position and Dmv is
the uncertainty in momentum, then
21Quantum Mechanics and Atomic Orbitals
- Schrödinger proposed an equation that contains
both wave and particle terms. - Solving the equation leads to wave functions.
- The wave function gives the shape of the
electronic orbital. - The square of the wave function, gives the
probability of finding the electron, - that is, gives the electron density for the atom.
22Electron Density Distribution
Probability of finding an electron in a hydrogen
atom in its ground state.
23The Three Quantum Numbers
- Schrödingers equation requires 3 quantum
numbers - Principal Quantum Number, n. This is the same as
Bohrs n. As n becomes larger, the atom becomes
larger and the electron is further from the
nucleus. (n 1, 2, 3) - Azimuthal Quantum Number, l. This quantum number
depends on the value of n. The values of l begin
at 0 and increase to (n - 1). We usually use
letters for l (s, p, d and f for l 0, 1, 2, and
3). Usually we refer to the s, p, d and
f-orbitals. (l 0, 1, 2n-1). Defines the shape
of the orbitals. - Magnetic Quantum Number, ml. This quantum number
depends on l. The magnetic quantum number has
integral values between -l and l. Magnetic
quantum numbers give the 3D orientation of each
orbital in space. (m -l01)
24Orbitals and Quantum Numbers
25Class Guided Practice Problem
- (a) For n 4, what are the possible values of l?
(b) For l 2. What are the possible values of
ml? What are the representative orbital for the
value of l in (a)?
Class Practice Problem
- (c) How many possible values for l and ml are
there when (d) n 3 (b) n 5?
26Representations of Orbitals The s-Orbitals
- All s-orbitals are spherical.
- As n increases, the s-orbitals get larger.
- As n increases, the number of nodes increase.
- A node is a region in space where the probability
of finding an electron is zero. - At a node, ?2 0
- For an s-orbital, the number of nodes is (n - 1).
27The s-Orbitals
28The p-Orbitals
- There are three p-orbitals px, py, and pz.
- The three p-orbitals lie along the x-, y- and z-
axes of a Cartesian system. - The letters correspond to allowed values of ml of
-1, 0, and 1. - The orbitals are dumbbell shaped.
- As n increases, the p-orbitals get larger.
- All p-orbitals have a node at the nucleus.
29The p-Orbitals
Electron-distribution of a 2p orbital.
30The d and f-Orbitals
- There are five d and seven f-orbitals.
- Three of the d-orbitals lie in a plane bisecting
the x-, y- and z-axes. - Two of the d-orbitals lie in a plane aligned
along the x-, y- and z-axes. - Four of the d-orbitals have four lobes each.
- One d-orbital has two lobes and a collar.
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32Orbitals and Quantum Numbers
- Orbitals can be ranked in terms of energy to
yield an Aufbau diagram. - As n increases, note that the spacing between
energy levels becomes smaller. - Orbitals of the same energy are said to be
degenerate.
33Orbitals and Their Energies
34Electron Spin and the Pauli Exclusion Principle
- Line spectra of many electron atoms show each
line as a closely spaced pair of lines. - Stern and Gerlach designed an experiment to
determine why. - A beam of atoms was passed through a slit and
into a magnetic field and the atoms were then
detected. - Two spots were found one with the electrons
spinning in one direction and one with the
electrons spinning in the opposite direction.
35Electron Spin and the Pauli Exclusion Principle
36Electron Spin and the Pauli Exclusion Principle
- Since electron spin is quantized, we define ms
spin quantum number ? ½. - Paulis Exclusions Principle no two electrons
can have the same set of 4 quantum numbers. - Therefore, two electrons in the same orbital must
have opposite spins.
37Electron Configurations Hunds Rule
- Electron configurations tells us in which
orbitals the electrons for an element are
located. - Three rules
- electrons fill orbitals starting with lowest n
and moving upwards - no two electrons can fill one orbital with the
same spin (Pauli) - for degenerate orbitals, electrons fill each
orbital singly before any orbital gets a second
electron (Hunds rule).
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40Electron Configurations and the Periodic Table
- The periodic table can be used as a guide for
electron configurations. - The period number is the value of n.
- Groups 1A and 2A (1 2) have the s-orbital
filled. - Groups 3A - 8A (13 - 18) have the p-orbital
filled. - Groups 3B - 2B (3 - 12) have the d-orbital
filled. - The lanthanides and actinides have the f-orbital
filled.
41Class Guided Practice Problem
- Write the electron configurations for the
following atoms (a) Cs and (b) Ni
Class Practice Problem
- Write the electron configurations for the
following atoms (a) Se and (b) Pb
42Condensed Electron Configurations
- Neon completes the 2p subshell.
- Sodium marks the beginning of a new row.
- So, we write the condensed electron configuration
for sodium as - Na Ne 3s1
- Ne represents the electron configuration of
neon. - Core electrons electrons in Noble Gas.
- Valence electrons electrons outside of Noble
Gas.
43Transition Metals
- After Ar the d orbitals begin to fill.
- After the 3d orbitals are full, the 4p orbitals
begins to fill. - Transition metals elements in which the d
electrons are the valence electrons.
44Lanthanides and Actinides
- From Cs onwards the 4f orbitals begin to fill.
- Note La Xe6s25d14f0
- Elements Ce - Lu have the 4f orbitals filled and
are called lanthanides or rare earth elements. - Elements Th - Lr have the 5f orbitals filled and
are called actinides. - Most actinides are not found in nature.