1 Atomic Structure Electron Configurations & Periodicity.
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Transcript of 1 Atomic Structure Electron Configurations & Periodicity.
1
Atomic StructureAtomic StructureElectron Configurations & Electron Configurations & PeriodicityPeriodicity
Slide 2
Introduction Atomic structure explains chemical properties
and patterns of chemical reactivity. Chemical reactions involve electrons. Knowing
where the electrons are, how many, and what their energy levels helps explain many chemical phenomena.
Spectroscopy is used to explore atomic structure. Because of this, we start with a discussion of the nature of light.
Slide 3
The Nature of LightParticles or Waves??
Light must be made of particles because it… travels in a vacuum reflects off of objects exerts force (on the
tails of comets) Light must consist of
waves because it… reflects like waves refracts and diffracts exhibits interference
By the end of the 19th century,scientists had concluded that light is composed of WAVES!
Slide 4
Electromagnetic Radiation Visible light is just one form of electromagnetic
radiation Light propagates in space as a wavewave In vacuum, speed of light is constant and given
the symbol “c”, c = 3.00 x 108 m/s Light waves have amplitude, frequency, and
wavelength. = wavelength - distance between consecutive
crests, = frequency, # of crests that pass a given point in one second (SI Unit is s-1 or Hz)
c = c = and = c/
Slide 5
James Maxwell proposed in the mid-1800’s that light is composed of perpendicular electric and magnetic waves
Slide 6
are distances – S.I. unit is the meter
Which of the above waves has the higher frequency?
Slide 7
The 7 Regions of the E.M. Spectrum
Slide 8
Slide 9
Sample Calculation – wavelength/frequency conversion
Calculate the frequency of visible light having a wavelength of 485 nm?
Remember to use S.I. units in your calculations!
= c / = (3.00 x 108 m/s) ÷ (4.85 x 10-7 m) = 6.19 x 1014 s-1
What colour of visible light is this?
Slide 10
Sample Calculation – wavelength & frequency conversion
CO2 absorbs light with a wavelength of 0.018 mm. Which frequency is this?
Remember that 1 Hertz (Hz) 1 s-1
What is the wavelength of WFAE at 90.7 MHz?
8 113 1
3
c 3.00 10 ms1.7 10 s
0.018 10 m
8 1
6 1
c 3.00 10 ms3.31m
90.7 10 s
Slide 11
Particle Theory of Light In 1900, Max Planck turned the world of physics on
its head by resurrecting the particle theory of light. Planck was trying to explain the “ultraviolet
catastrophe” while studying blackbody radiation. He proposed that light is composed of particles
(quanta) each carrying a fixed amount of energy. The amount of energy per quantum is directly
proportional to the frequency of the light:
34hcE h or E , h 6.626 10 J s
34hc
E h or E , h 6.626 10 J s
Slide 12
Planck’s Equation – sample problem The wavelength of maximum visual acuity in
humans is 550 nm. (green light) What is the energy of a single photon having this
wavelength?
Ans. 3.61 x 10-19 J per photon
What is the energy of a mole of photons at 550 nm?
Ans. 218 kJ/mol
Slide 13
Energy, wavelength, frequency
a) X-Rays
b) Red light
c) Green light
d) Radio waves
Rank the above in order of … increasing wavelength decreasing energy increasing frequency
Slide 14
Atomic Emission Spectra“Line Spectra” vs “Continuous Spectra”
Historic work (1800’s) involving light emitted by pure elements in gas phase, subjected to very high voltages.
The light was passed through a prism or diffraction grating to produce a spectrum.
Each element emitted only certain wavelengths of light – a LINE SPECTRUM instead of the more familiar “continuous” spectrum seen in the rainbow.
Balmer and Rydberg described the lines mathematically, for hydrogen.
Hydrogen’s emission spectrum has several lines in the visible region – called the “Balmer series”
Slide 15
A Continuous Spectrumcontains all wavelengths of light – a rainbow
Slide 16
Slide 17
Bohr’s Explanation of Line Spectra
Neils Bohr developed a mathematical model that could explain the observation of atomic line spectra.
He proposed that electrons orbit the nucleus in certain “allowed” orbits - or energy levels. That is, the electron’s energy is QUANTIZED (not continuous).
Working on a model of single-electron atoms, Bohr derived an equation to calculate the energy of an electron in the nth orbit of such an atom:
218
22.18 10n
ZE
n
where Z = atomic number
and n = electron energy level
Slide 18
Bohr’s Quantum Model for Hydrogen
The electron in hydrogen occupies discrete energy levels.
The atom does not radiate energy when the electron is in an energy level.
When an electron falls to a lower energy level, a quantum of radiation is released with energy equal to the difference between energy levels.
An electron can jump to higher energy levels if the atom absorbs a quantum of radiation with sufficient energy.
Slide 19
The Hydrogen Line Spectrum
Slide 20
Bohr’s Model: Calculations
Show that an electron transition from n = 4 to n = 2 results in the emission of visible light. Calculate the wavelength of the light emitted.
Step 1: Calculate E4 & E2
E4 = -1.36 x 10-19 J
E2 = - 5.45 x 10-19 J
Step 2: Find E42
E = E2 – E4 = 4.09 x 10-19 J
Step 3: Calculate = 4.86 x 10-7 m = 486 nm
Slide 21
What’s Wrong with Bohr’s Model??
Although it works great for single-electron atoms, Bohr’s model fails for atoms with 2 or more electrons!
It was a huge leap forward, but was fundamentally flawed.
Ultimately, the failure of Bohr’s model lay in the fact that he treated the electron as a charged particle orbiting the nucleus like a planet around the sun.
Electrons are more complicated …
Slide 22
Wave-Particle Dual Nature of Electrons
Einstein’s famous equation, E = mc2, suggests that energy and mass are related – one can convert matter directly into energy.
Louis de Broglie made the leap that if light can behave as wave/particles, then so can matter!
He showed that the wavelength of a baseball is negligible (as expected), but that the wavelength of an electron was on the order of magnitude equal to that of electromagnetic radiation!
This is what Bohr had missed – an atomic model must make use of the wave-nature of electrons to be complete!
Slide 23
Visualizing the Wave-Nature of Electrons
Slide 24
Heisenberg’s “Uncertainty Principle” The more precisely the position is
determined, the less precisely the momentum is known in this
instant, and vice versa.
It is impossible to determine BOTH the position and momentum (velocity) of an electron - the act of observing the electron changes it.
The electron exists in nature as a wave-particle (whatever that is) until an experimenter observes it and imposes one of the two natures upon it!
25
"When it comes to atoms, language can only be used as in poetry. The poet too, is not nearly so concerned with describing facts as with creating images."
- Niels Bohr to Werner Heisenberg
Slide 26
The Heisenburg uncertainty principle is the catch 22 of physics. Most modern physics and chemistry is largely based on the study of electrons. In order to view an electron we must use light to observe it, but in the process of observing we change the electron’s momentary existence because the light necessary to view it takes the form of a photon particle. The photon particle travels at approximately the same velocity as the electron particle, so that when it impacts the electron it alters its position as when two asteroids collide into each other at similar velocities but different angles.
Therefore, according to Heisenburg, it is impossible to know decisively an electron’s position and momentum.
Slide 27
Heisenburg proposed that this inability to perceive reality on an atomic level is not the result of technological ignorance, but rather a fact of the laws of nature. In other words, Heisenburg believed that no matter how technologically advanced we become we would never be able to fully perceive and record atomic reality. This means that an electron’s orbital path around the nucleus of an atom can only be statistically approximated.
This is why the quantum atomic model has a cloud of electrons, not a few electrons following exact elliptical orbits as in Bohr's atomic model. Each electron in the quantum atomic model is a calculated probability, so the cloud describes not the exact orbit of millions of electrons, but rather the probability of the position of only a few electrons at any given time.
Slide 28
The Schrödinger Wave Equation Schrödinger applied de Broglie’s concept of
matter waves to the electron He explained the quantum energies of the
electron orbits in the Bohr model of the atom as vibration frequencies of electron "matter waves" around the atom's nucleus.
He provided a mathematical equation (wave function) to describe electron waves.
Physicists had difficulty explaining the MEANING of the wave function itself, but it turns out that its square gives the probabilityprobability of finding the electron in a particular region of space in the atom.
Slide 29
Schrodinger Equation, cont. These regions of probability are called orbitals, orbitals, and this
concept replaces that of the electron “orbit”. Instead of electrons orbiting like planets around the sun,
Schrodinger’s picture shows an “electron cloud” surrounding the nucleus and doesn’t state anything about the path or position of electrons within that cloud.
Orbital “pictures” shown in texts represent regions of space where the probability of finding an electron is 90% or greater.
Slide 30
Quantum Numbers Schrodinger's wave equation used three constants
(“quantum numbers”) that were used to describe orbitals – regions of space where an electron has a probability of being found.
His equation used 3 quantum numbersquantum numbers to describe the size & energy, shape, and orientations of the orbitals in atoms.
The three quantum numbers: n, l and ml . This set of three numbers provides us with an “orbital
address” for an electron within an atom – we can describe the orbital in which an electron is found if we know these three quantum numbers.
Slide 31
Principal Quantum Number, n
n can have values > 1, integers only. For element atoms on the periodic table in their
ground statesground states, 1 n 6 As n increases, energy of electron increases and
size of orbital increases Larger n means greater probability of greater
distance from the nucleus. Electrons with same value of n are said to be in
the same “electron shell”
Slide 32
Shape Quantum Number, l The values for l (lower case letter L, script) are limited by
the principal energy level – they range from 0 to “n–1” Example: If n = 3, l can be 0, 1 or 2
l gives information about shape of orbital
l = 0 s orbital (found on all principle energy levels)
l = 1 p orbitals (found on level 2 and higher)
l = 2 d orbitals (found on level 3 and higher)
l = 3 f orbitals (found on level 4 and higher)
Slide 33
s Orbitals on three energy levels
NODE
Graphs show Probability vs Distance from nucleus
Graphs show Probability vs Distance from nucleus
Slide 34
p and d Orbital shapes
Slide 35
Slide 36
Orientation Quantum Number, ml The values of ml are limited by the value of l for
a given orbital. They include positive and negative integers from -l through +l , inclusive
For a p orbital, l = 1 , so ml can be: 1, 0, 1
ml gives information about orientationorientation of orbitals in space
The # of allowed values gives the number of orbitals of this type on a given energy level. (3, in the case of p orbitals)
Slide 37
Electron Spin Quantum Number, ms A fourth quantum number, ms
describes electron spinelectron spin (either +½ or –½)
Each electron in atom has a unique set of these four quantum numbers.
Electrons in orbitals with same n and l values are said to be in the same subshell.subshell.
Electrons with all three numbers the same, n, l , and ml , are in
the same orbital.
A spinning negative charge creates a magnetic field. The direction of spin d determines the direction of the field.
Slide 38
Pauli Exclusion Principle Electrons have negative charge and repel each
other. How are the electrons in an atom distributed?
Wolfgang Pauli proposed that no two electrons no two electrons in a given atom can be described by the in a given atom can be described by the same four quantum numbers!same four quantum numbers!
The first three quantum numbers determine an orbital – therefore spins must be opposite!
Practical resultPractical result is that each orbital can hold a maximum of two electrons, with opposite spins.
Slide 39
Concept Check Which of the following sets of
quantum numbers are NOT allowed in the hydrogen atoms? For those that are incorrect, state what is wrong.
n l mlms
2 1 -1 + ½
1 1 0 - ½
8 7 -6 + ½
1 0 2 - ½
What is the maximum number of electrons in an atom that can have these quantum numbers?
n = 4 n = 5, ml = +1
n = 5, ms = + ½
n = 2, l = 1 n = 3, l = 2 n = 3, ml = 4
Slide 40
Electron Configurations
Electrons orbitals are defined by their quantum numbers, n, l and ml .
Each electron in an atom has a unique set of 4 quantum numbers.
No two electrons can have the same “address”, i.e., the same 4 quantum #’s
Rules define how multiple electrons will be distributed among the possible energy levels
Slide 41
Aufbau Principle In the ground state, the electrons occupy the lowest
available energy levels. An atom is in an excited state if one or more electrons are in higher energy orbitals.
In atoms with more than one electron the lower energy orbitals get filled by electrons first!
This is the Aufbau principle, which is named after the German word which means “to build up”.
When one describes the locations of the electrons in an atom, start with the lowest energy electron and work up to the highest energy electron.
Slide 42
Hund’s Rule A set of orbitals is said to be “degenerate” if the orbitals
possess the same energies. For example, all three “2p” orbitals on energy level 2 are degenerate. All five “3d” orbitals on energy level 3 are also degenerate.
When filling a set of degenerate orbitals, Hund said that electrons should be left unpaired as long as possible so as to minimize electron-electron repulsions within the orbitals.
When each degenerate orbital has one electron, electrons will then pair, spins opposed, until that sub-shell is filled.
Slide 43
Summary of Distribution Rules Electrons distribute to lower energy levels
until they are filled, before occupying higher levels. (Aufbau Principle)
Electrons will spread out as much as possible within a sub-shell. (Hund’s Rule)
Electrons will pair up, two to an orbital, spins opposed, until that sub-shell is filled. (Pauli Exclusion)
Every electron will have unique set of 4 quantum numbers.
Slide 44
Electronic Configurations An electron configuration is a way of describing the
locations of electrons within an atom. Usually written for the ground state of an atom: when its
electrons occupy orbitals giving the lowest possible overall energy for the atom
Each subshell is designated by “n” and the type of orbital. Such as: 1s 3p 4d
The number of electrons in an orbital is shown as a superscript: 1s2 3p3 4d9
How does one determine the order of filling of the orbitals in an atom?? Which orbitals get filled first??
Slide 45
Orbital Energies in Multielectron Atoms
Slide 46
The Order of Filling of OrbitalsSimply follow the order of elements in the periodic table!
Slide 47
Another useful device…
Start at the top and follow the arrows: 1s, 2s, 2p, 3s, 3p, 4s, 3d, 4p, 5s…
Slide 48
Examples of Electron Configurations Helium has 2 electrons in the 1s orbital, He: 1s2
Carbon has 6 electrons, C: 1s2 2s2 2p2
Calcium has 20 electrons, Ca: 1s2 2s2 2p6 3s2 3p6 4s2
Calcium cation, Ca2+: 1s2 2s2 2p6 3s2 3p6 Sulfide anion, S2–: 1s2 2s2 2p6 3s2 3p6
Notice that the superscripts add up to the total number of electrons on the atom or ion! Each of these examples represents the “ground state” of the atom/ion because the electrons are in the lowest possible energy levels.
Slide 49
Orbital Diagrams
Slide 50
Noble Gas “shorthand” Notation The core electrons can be indicated by a short
form: use the last noble gas to indicate filled shells.
Find the last noble gas before the element under consideration. Start the electron configuration with the symbol for this noble gas element and just tack on the extra electrons:
Ca: 1s2 2s2 2p6 3s2 3p6 4s2
Ca: [Ar] 4s2
Ar: 1s2 2s2 2p6 3s2 3p6
Slide 51
There Have to be EXCEPTIONS As atoms get larger, their
outermost electrons become closer in energy
Large atoms have “exceptions” to the Aufbau Principle in the locations of their valence electrons. We will memorize two: Cr and Cu
Transition metal cations are also strange in their electron configurations
Cr: [Ar] 4s1 3d5
Cu: [Ar] 4s1 3d10
In both cases, one of the 4s electrons is promoted to the “3d” subshell.
Fe2+: [Ar] 3d6
Cu2+: [Ar] 3d9
Notice that the 4s electrons are lost before the 3d electrons!
Slide 52
Paramagnetism & Diamagnetism An atom is said to be
paramagnetic if it possesses unpaired electrons.
These electrons will result in the atom possessing a net magnetic field
It will then be attracted into an external magnetic field
An atom is diamagnetic if all its electrons are paired – it will NOT possess a net magnetic field because each electron’s field will be cancelled
These atoms are NOT attracted into an external magnetic field
What is “ferromagnetism”?
Slide 53
Testing for ParamagnetismSee Kotz & Treichel page 290
Slide 54
Electron ConfigurationCauses Periodic Trends “Periodicity” refers to similarities in behavior and
reactivity due to similar outer shell electron configurations.
All the Alkali Metals have one unpaired valence electron; all the Noble Gases have completely filled subshells
We will examine periodic trends in atomic radius, ionization energy, electronegativity, and electron affinity
Slide 55
“Valence Electrons”
Valence electrons are those electrons in the highest principal energy level within an atom - the s and p electrons in the outermost shell of an atom in its ground state.
These are the electrons involved in forming bonds with other atoms during chemical reactions.
Most common oxidation states (ion charge) for the element can be derived from valence electrons
Completely filled, half filled and empty sub-shells have special stability (not sure why!?)
Slide 56
Valence Configurations
The “valence configuration” is that part of an electron configuration that describes the valence electrons.
For example, sodium’s valence configuration is just “3s1”.
The valence configuration of bromine is “4s24d5”. We leave out the “3d10” electrons because they are not in the outermost principal energy level.
Slide 57
Periodic Trends: Atomic Size Properties of elements and their ions are
determined by electron configurations Individual atoms cannot be accurately
measured. Atomic sizes are determined from bond
lengths of compounds with various atoms
Br-Br2.28 Ar = 1.14 A
Br-C1.91 Arcarbon = 1.91-1.14 = 0.77 A
Slide 58
Atomic Size, cont. Atomic radii increase within a group (column) as
the principal quantum number of outermost shell increases
Electrons of outermost shells have greater probability of being farther from the nucleus
Atomic size decreases across a row (period) from Left to Right, because the effective nuclear charge increases. There are more and more protons in the nuclei
attracting more and more electrons!
Slide 59
Atomic Radii:Atomic Radii:
Atoms get larger as you move down a group
Atoms get smaller as you go across a period
Slide 60
Slide 61
Ionization Energies First Ionization energy: energy required to
remove an electron from the ground state atom in the gaseous state to make a cation
1st ionization of Mg:
Mg Mg+ I.E. = 738 J/mol
[Ne]3s2 [Ne]3s1
2nd ionization of Mg
Mg + Mg2+ 1450 J/mol
[Ne]3s1 [Ne]
Slide 62
Trend in First Ionization Energies First ionization energies decrease down a group
as radii increase: Na > K > Cs First ionization energies increase across a row
as radii decrease: Li < F < Ne For similar reasons that explained trends in
atomic radii. For a given element, IE2 always > IE1 because of
the same # protons in nucleus holding onto fewer electrons.
Slide 63
Slide 64
Trends in First Ionization Energies
Slide 65
First Ionization Energy (cont’d) Lowest IE1 are in the
lower left corner of periodic table (Fr and Cs)
Irregularities in IE1 trends arise from special electron configurations.
Half filled sub-shells are especially stable: every orbital has only one electron.
Oxygen has slightly lower IE1 than nitrogen because it takes more energy to disrupt N’s half-filled orbital configuration
Boron has slightly lower IE1 than Beryllium because its first electron is removed from the p-subshell further from the nucleus than the first electron removed in Be
Slide 66
Electron Affinity Energy change when a gas phase atom gains an
electron to become an anion.
Cl (g) + e- Cl– (g) EA = – 349 kJ/mol
The more negative an EA, the greater the affinity for electrons!
Electron affinities “tend” to become more negative across a period and less negative moving down a group
EA least negative for alkaline earth and noble gas elements: they have full or half full s- or p-orbitals and it would take a lot of energy to add another electron
Slide 67
Slide 68
Slide 69
Slide 70
Ion Sizes Cations: radius is always smaller than the
neutral atom. Loss of electrons (to make cation) leaves fewer
electrons attracted to same # of protons OR….. loss of outermost shell altogether as in
group 1A [Ne]3s1 [Ne] for sodium Anions: radius is always larger than neutral
atom. Same # protons pulling on more electrons;
also electrons repel each other.
Slide 71
Slide 72
Isoelectronic Atoms and Ions Isoelectronic atoms or ions have same electron configurations – the same number of electrons in same orbitals
Na+ , Ne and F- are isoelectronic: 1s2 2s2 2p6
For isoelectronic atoms and ions, the species with the most protons will be smallest
It has greater nuclear attraction for the same number of electrons, so the electron shells will be pulled closer to nucleus.
73
Bonding in Molecules
Ionic Bonds
Polar Covalent Bonds
Non-Polar Covalent Bonds
Slide 74
Definitions
ELECTRONEGATIVITY is the attraction an atom has for electrons in a chemical bond.
A POLAR BOND is one between atoms with different electronegativities - one atom attracts electrons more strongly than the other. As a result, one atom acquires a partial positive charge and the other a partial negative charge.
Slide 75
More Definitions
A DIPOLE is a separation of charge. A polar bond is an example of a dipole.
A DIPOLE MOMENT is the magnitude of a dipole - it depends on the size of the charges involved.
A POLAR MOLECULE is one that possesses an overall dipole moment.
Slide 76
Classifying Chemical Bonds
IONIC bonds are characterized as… bonds between metals and non-metals bonds between cations and anions bonds involving a transfer of electrons (from a
metal to a non-metal)
The best classification of an ionic bond uses the concept of electronegativity.
Slide 77
Classifying Chemical Bonds
An ionic bond forms between two atoms with a large difference in electronegativity - usually stated as being greater than about 1.7 Paulings.
e.g. NaCl: difference is 2.0 Paulings e.g. CuO: difference is 1.7 Paulings
Slide 78
Classifying Chemical Bonds
COVALENT bonds are usually described as… bonds between two non-metal atoms bonds involving a sharing of electrons
Using the concept of electronegativity, we can see that there are two types of covalent bonds.
Slide 79
Classifying Chemical Bonds
POLAR COVALENT BONDS result from unequal sharing of electrons by atoms that creates a small dipole.
This type of bond occurs when there is a small but significant difference in electronegativity - between 0.4 and 1.7 Paulings. e.g. N-H: diff is 0.9 Paulings e.g. Cu-S: diff is 0.7 Paulings
Slide 80
Classifying Chemical Bonds
NON-POLAR COVALENT BONDS result from an equal sharing of electrons.
There is no dipole created since the electrons are shared equally.
This bond forms between atoms with similar (or the same) electronegativities - differences between 0 and 0.4 Paulings.
Slide 81
Exercise
Classify the following chemical bonds. Show your work. Li-F Br-Br Fe-O Al-Cl C-S C-H
Slide 82
Polarity of Molecules
A diatomic molecule (e.g. HF) will be polar if its bond is polar.
Larger molecules are polar only when the following criteria are met: they possess at least one polar bond their geometries do not result in the dipoles
cancelling each other out! (e.g. CO2)