Title: Chapter 13 Electrons in Atoms
1Chapter 13 Electrons in Atoms
2I. Models of the AtomA. The Evolution of
Atomic Models
- 1. There are four major models of the atom that
have been developed from John Dalton theory. - 2. Dalton Atomic Theory a. He theorized that
an atom was indivisible, uniformly dense
sphere. b. He theorized that all atoms of the
same element have the same mass and the same
chemical behaviors. c. He theorized that atoms
of different elements have different chemical
behaviors. d. He theorized that atoms of
different elements combine to form compounds.
(Example H2O)
3I. Models of the AtomA. The Evolution of
Atomic Models
- 3. J.J. Thomson realized that the accepted model
did not take electrons into account. a. He is
credited with the discovery of the negatively
charged particles called electrons. b. He
theorized that the atom is a dense sphere with a
positive charge and also contains negative
charged particles. c. His model is also known
as the Plum Pudding model.
4I. Models of the AtomA. The Evolution of
Atomic Models
- 4. Ernest Rutherford expanded on Thomsons
theory. a. The atom has a very dense center of
positive charge called the nucleus. b. The
nucleus contains the protons for the atom and
make up more than 99.9 of its mass. c. The
electrons surround the nucleus.
5I. Models of the AtomA. The Evolution of
Atomic Models
- 5. Niels Bohr proposed a model in which the
electrons move around the nucleus. a. He
theorized that the electron orbits the
nucleus. b. He theorized that the orbits were
different energy levels that the electrons travel
in and can be excited to a high energy level. c.
He theorized that the electrons did not lose
energy and fall into the nucleus. (The weakness
in Rutherfords theory.)
6I. Models of the AtomA. The Evolution of
Atomic Models
- 6. A quantum of energy is the amount of energy
required to move an electron from its present
energy level to the next higher one. (Also called
a quantum leap)
7I. Models of the AtomB. The Quantum Mechanical
Model
- 1. Erwin Schrödinger related the amplitude of
the electron wave, Y (psi), to any point in
space around the nucleus. 2. His equation
treated the electron as a wave and developed an
equation to describe this behavior.
8I. Models of the AtomB. The Quantum Mechanical
Model
- 3. The quantum mechanical model comes from the
mathematical solutions to Schrödinger
equation.4. The quantum mechanical model does
not define an exact path for the electron to take
around the nucleus but instead estimates a
probability of finding the electron in a certain
position.5. Since the volume occupied by an
electron is somewhat vague, it is better to
refer to an electron cloud.
9I. Models of the AtomB. The Quantum Mechanical
Model
10I. Models of the AtomC. Atomic Orbitals
- 1. Electrons can occupy only specific energy
levels.2. These energy levels, referred to as
n is called the principal quantum number.3.
The maximum number of electrons that a level can
contain is 2n2 (Whole number integers only).
11I. Models of the AtomC. Atomic Orbitals
- 4. These are referred to as sublevels and the
number of sublevels for each energy level is
equal to the value of the principal quantum
number.5. The lowest energy level is s.6.
The second lowest is p ,the third lowest level
is d, and the remain level is f.
12I. Models of the AtomC. Atomic Orbitals
- 7. The s orbital is spherical in shape and
contains 2 electrons and is also called the
ground state. 8. The p level is barbell shape
and exist along the axis of the plane.9. The
d orbitals exist in the plane. 10. The s
level contains 1 pair of electrons, p contains
3 pairs, d contains 5 pairs, and f contains
7 pairs.
13II. Electron Arrangement in AtomsA. Electron
Configurations
- 1. The ways in which electrons are arranged
around the nucleus is called electron
configuration.2. The are three rule that tell
you how to find the configurations. a. Aufbau
principle - b. Pauli Exclusion principle
- c. Hunds Rule
14II. Electron Arrangement in AtomsA. Electron
Configurations
- 2a This is called the Aufbau principle. 1.
Electrons enter at the lowest energy level. 2.
Some energy levels overlap into the adjacent
principal energy level.
15II. Electron Arrangement in AtomsA. Electron
Configurations
16II. Electron Arrangement in AtomsA. Electron
Configurations
- 2b. This is called the Pauli exclusion
principle. 1. Spectral data shows that only 2
electrons can exist in the same orbital. 2.
Electrons behave as if they were spinning about
their own axis. 3. When electrons occupy the
same orbital they are said to spin in opposite
directions (assign 1/2 and 1/2).
17II. Electron Arrangement in AtomsA. Electron
Configurations
- 2c. This is called Hunds Rule. 1. Also with
the principle, you must have all orbital filled
with one electron before you can add the other
electron with opposite spin to the orbital. 2 .
All elements would like to have a completely
filled orbital and the maximum number of
electrons that can exist in a filled orbital is
eight.
18II. Electron Arrangement in AtomsA. Electron
Configurations
- 3. When writing electron configurations, you
must know the total number of electrons for the
element (atomic number).4. Write down the
sequence of orbitals.5. Draw circle to
represent the orbitals.6. Place arrows (or
slashes) to represent the electrons.
19II. Electron Arrangement in AtomsA. Electron
Configurations
20II. Electron Arrangement in AtomsA. Electron
Configurations
21II. Electron Arrangement in Atoms B. Exceptional
Electron Configurations
- 1. Filled sublevels are more stable than partial
filled or half-filled sublevels. 2. But
sometimes half-filled may be more stable than
other configurations.
22III. Physic and the Quantum Mechanical ModelA.
Light and Atomic Spectra
- 1. This energy consist of variation in electric
and magnetic fields taking place in a regular,
repeating fashion. (Electromagnetic energy)2.
Light is a form of electromagnetic radiation
23III. Physic and the Quantum Mechanical ModelA.
Light and Atomic Spectra
- 3. If you plot the strength of the variation
against time, the graph shows waves of
energy.4. The number of waves peaks that occur
in a unit of time is called the frequency of the
wave (Greek letter v and units are Hertz (Hz)).
24III. Physic and the Quantum Mechanical ModelA.
Light and Atomic Spectra
- 5. The distance between the peaks is the
wavelength (Greek letter ?) and the amplitude of
a wave is the height from the maximum
displacement from zero.6. These characteristics
of waves are related by the statement c ?v
where c is the speed of light which is 3.0 x 10
8 m/s.
25III. Physic and the Quantum Mechanical ModelA.
Light and Atomic Spectra
- 7. The wavelengths of light can separate into a
spectrum of colors.8. This is part of the
visible spectrum.9. There are two types of
spectrums. a. Adsorption spectrum. b.
Emission spectrum.
26III. Physic and the Quantum Mechanical ModelA.
Light and Atomic Spectra
- 10. Adsorption spectrum is when the energy
gained by the excited electron is is absorbed so
that it is missing in visible spectrum.11.
Emission spectrum is when the excited electrons
lose the energy and it is emitted at specific
points on the visible spectrum that appear as
single lines on a detector.
27III. Physic and the Quantum Mechanical ModelB.
The Quantum Concept and the Photoelectric Effect
- 1. Max Planck used Bohrs theory to develop his
hypothesis.2. He assumed that energy is given
off in packets called quanta or photons instead
of a steady stream.
28III. Physic and the Quantum Mechanical ModelB.
The Quantum Concept and the Photoelectric Effect
- 3. He stated that the amount of energy given
off is related to the frequency of light (v -
Greek letter nu).4. He thought a quantum energy
was equal to E hv where h is the constant 6.63
x 10 -34 J/Hz (Hz Hertz).
29III. Physic and the Quantum Mechanical ModelB.
The Quantum Concept and the Photoelectric Effect
- 5. Albert Einstein proposed that light could be
described as a quanta of energy that behaved as
if they were particles. 6. The dual
wave-particle behavior is called the
photoelectric effect.
30III. Physic and the Quantum Mechanical ModelB.
The Quantum Concept and the Photoelectric Effect
- 7. In the photoelectric effect, metals eject
electrons when light shines on them.8. The
frequency and the wavelength of the light
determine if the photoelectric effect will occur.
31III. Physic and the Quantum Mechanical ModelC.
An Explanation of Atomic Spectra
- 1. Consider the electron of a hydrogen atom in
its lowest energy level, or ground state.2. The
quantum numbers represent the different energy
states.
32III. Physic and the Quantum Mechanical ModelC.
An Explanation of Atomic Spectra
- 3. The difference between these energy states
corresponds to the lines in the hydrogen
spectrum.4. With more complex atoms more than
one electron is present and the interaction
between electrons make solution to the equation
impossible because electrons have the same charge.
33III. Physic and the Quantum Mechanical ModelC.
An Explanation of Atomic Spectra
- 5. It is possible to approximate the electronic
structure of a multi-electron atom.6. This
approximation is made by first calculating the
various energy states and quantum numbers.7.
It is assumed that the various electrons in
multi-electron atom occupy the same energy states
without affecting each other.
34III. Physic and the Quantum Mechanical ModelD.
Quantum Mechanic
- 1. Louis De Broglie proposed an idea based on
Plancks theory and Einsteins relationship of
matter and energy.2. Using the two formulas, he
equated mc2 h? (v frequency).
35III. Physic and the Quantum Mechanical ModelD.
Quantum Mechanic
- 3. He substituted v for the velocity of light
(c) so that mv 2 hv and v /? for v to get
mv 2 hv /?. (? - Lamda wavelength)4. To
determine wavelength (?), the equation becomes ?
h/mv .
36III. Physic and the Quantum Mechanical ModelD.
Quantum Mechanic
- 5. This allows for predictions of the
wavelength of a particles.6. Werner Heisenburg
refined ideas about atomic structure.7. He
stated that it is impossible to know the exact
position and momentum of an electron in an atom.
37III. Physic and the Quantum Mechanical ModelD.
Quantum Mechanic
- 8. Using the equation for momentum, he proposed
that mv p where m is mass and p is momentum.
9. The uncertainty of position and momentum are
related to Plancks constant ?p ?x gt h where p
is momentum and x is position (? change).10.
Because h is constant, ? p and ? x are inversely
proportional to each other.