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10/29/2018
1
CHAPTER 3Atomic Structure:Explaining the Properties of Elements
We are going to learn about the electronic structure of the atom,
and will be able to explain many things, including atomic
orbitals, oxidation numbers, and periodic trends.
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Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
The Electromagnetic SpectrumContinuous range of radiant energy,
(also called electromagnetic radiation).
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Electromagnetic RadiationMutually propagating electric and magnetic fields, at right
angles to each other, traveling at the speed of light c
Speed of light (c) in vacuum = 2.998 x 108 m/s
a) Electricb) Magnetic
Properties of Waves - in the examples below,
both waves are traveling at the same velocity
Long wavelength = low frequency
Short wavelength = high frequency
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Units: wavelength = meters (m)
frequency = cycles per second or Hertz (s-1)
wavelength (m) x frequency (s-1) = velocity (m/s)
· u = wavelength, = frequency, u = velocity
Example:A FM radio station in Portland has a carrier wave frequency of 105.1 MHz. What is the wavelength?
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Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
Atomic Emission (Line) Spectra
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Blackbody Radiation
Photoelectric Effect• phenomenon of light striking a metal surface and
producing an electric current (flow of electrons).
• If radiation below threshold energy, no electrons released.
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Explained by a new theory: Quantum Theory
Blackbody Radiation and the Photoelectric Effect
• Radiant energy is “quantized”– Having values restricted to whole-number
multiples of a specific base value.
• Quantum = smallest discrete quantity of energy.
• Photon = a quantum of electromagnetic radiation
Quantized States
Quantized states: discrete energy levels.
Continuum states: smooth transition between levels.
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The energy of the photon is given by Planck’s Equation.
E = h h = 6.626 × 10−34 J∙s
(Planck’s constant)
Sample Exercise 7.2What is the energy of a photon of red light that has a wavelength of 656 nm? The value of Planck’s constant (h) is 6.626 × 10-34 J . s, and the speed of light is 3.00 × 108 m/s.
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Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
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The Hydrogen Spectrum and the Rydberg Equation
22
12 11100971
1
fi nn . =
λnm
Exercise 7.4: using the Rydberg Equation
What is the wavelength of the line in the emission spectrum of Hydrogen corresponding from ni = 7 to nf = 2?
22
12 11100971
1
fi nn . =
λnm
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Using the Rydberg Equation for Absorption
What is the wavelength of the line in the absorption spectrum of Hydrogen corresponding from ni = 2 to nf = 4?
22
12 11100971
1
fi nn . =
λnm
Neils Bohr used Planck and Einstein’s ideas of photons and quantization
of energy to explain the atomic spectra of hydrogen
+
n = 1
n = 2
n = 3
photon of
light (h)
n = 1
n = 2
n = 3
absorption emission
hh
n = 4
The Bohr Model of Hydrogen
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Electronic States
• Energy Level:
• An allowed state that an electron can occupy in an atom.
• Ground State:
• Lowest energy level available to an electron in an atom.
• Excited State:
• Any energy state above the ground state.
“Solar system” model of the atom where each “orbit”
has a fixed, QUANTIZED energy given by -
where n = “principle quantum number” = 1, 2, 3….
This energy is exothermic because it is potential
energy lost by an unbound electron as it is attracted
towards the positive charge of the nucleus.
En=−2.178686 x 10−18 Joules
n2
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E = h
E = h
Ephoton = DE = Ef - Ei
The Rydberg Equation can be derived from Bohr’s theory -
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Example DE Calculation
Calculate the energy of a photon absorbed when an electron is promoted from ni = 2 to nf = 5.
Sample Exercise 3.5
How much energy is required to ionize a ground-state hydrogen atom? Put another way, what is the ionization energy of hydrogen?
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Strengths and Weaknesses of the Bohr Model
• Strengths:• Accurately predicts energy needed to remove an
electron from an atom (ionization).
• Allowed scientists to begin using quantum theory to explain matter at atomic level.
• Limitations:• Applies only to one-electron atoms/ions; does not
account for spectra of multielectron atoms.
• Movement of electrons in atoms is less clearly defined than Bohr allowed.
Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
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Light behaves both as a wave and a particle -
Classical physics - light as a wave:
c = = 2.998 x 108 m/s
Quantum Physics -
Planck and Einstein:
photons (particles) of light, E = h
Several blind men were asked to describe an elephant. Each tried to determine
what the elephant was like by touching it. The first blind man said the elephant
was like a tree trunk; he had felt the elephant's massive leg. The second blind
man disagreed, saying that the elephant was like a rope, having grasped the
elephant's tail. The third blind man had felt the elephant's ear, and likened the
elephant to a palm leaf, while the fourth, holding the beast's trunk, contended
that the elephant was more like a snake. Of course each blind man was giving a
good description of that one aspect of the elephant that he was observing, but
none was entirely correct. In much the same way, we use the wave and particle
analogies to describe different manifestations of the phenomenon that we call
radiant energy, because as yet we have no single qualitative analogy that will
explain all of our observations.
http://www.wordinfo.info/words/images/blindmen-elephant.gif
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Standing Waves and Nodes
Not only does light behave like a particle
sometimes, but particles like the electron
behave like waves! WAVE-PARTICLE
DUALITY
Combined these two equations:
E = mc2 and E = h, therefore -
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The DeBroglie wavelength explains why only certain
orbits are "allowed" -
a) stable b) not stable
Sample Exercise 3.6 (Modified): calculating the wavelength of a particle in motion.
(a)Calculate the deBroglie wavelength of a 142 g baseball thrown at 44 m/s (98 mi/hr)
(b)Compare to the wavelength of an electron travelling at 2/3’s the speed of light. Mass electron = 9.11 x 10-31 kg.
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Using the wavelike properties of the electron.
Close-up of a milkweed bug Atomic arrangement of a Bi-Sr-
Ca-Cu-O superconductor
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Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers NOTE: will do Section 3.7 first3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
The electron as a Standing Wave
E. Schrödinger (1927)
mathematical treatment results in a “wave function”,
= the complete description of electron position and energy
electrons are found within 3-D “shells”, not 2-D Bohr orbits
shells contain atomic “orbitals” (s, p, d, f)
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Each orbital can hold up to 2 electrons
The probability of finding the electron = 2
Probabilities are required because of “Heisenberg’s Uncertainty Principle”
The electron as a Standing Wave
E. Schrödinger (1927)
We can never SIMULTANEOUSLY know with absolute
precision both the exact position (x), and momentum
(p = mass·velocity or mv), of the electron.
Dx·D(mv) h/4Uncertainty in
momentum
Uncertainty in
position
If one uncertainty gets very small, then the other becomes
corresponding larger. If we try to pinpoint the electron momentum,
it's position becomes "fuzzy". So we assign a probability to where the
electron is found = atomic orbital.
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If an electron is moving at 1.0 X 108 m/s with an uncertainty in
velocity of 0.10 %, then what is the uncertainty in position?
Dx 6 x 10-10 m or 600 pm
∆x∙∆ mv ≥h
4π
∆x ≥h
4π ∆ mv
∆x ≥h
4π m∆v
∆x ≥6.63 x 10−34Js
4π (9.11 x 10−31 kg)(.001 x 1 x 108 m/s)
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+
n = 1
n = 2
n = 3
1s
2s
3s
Orbitals are found in 3-D shells
instead of 2-D Bohr orbits. The Bohr
radius for n=1, 2, 3 etc was correct,
however.
+
n = 1
n = 2
n = 3
3px 3py 3pz
2px 2py 2pz
Do not appear until the 2nd shell and higher
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+
n = 1
n = 2
n = 3
Do not appear until the 3rd shell and higher
“The Shell Game”
(n = 1)
+
n = 1
n = 2
n = 3
In the first shell there is
only an s "subshell"
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“The Shell Game”
n = 2
+
n = 1
n = 2
n = 3
In the second shell
there is an s "subshell"
and a p "subshell"
“The Shell Game”
n = 3
+
n = 1
n = 2
n = 3
In the third shell
there are s, p, and d
"subshells"
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“f” Orbitals don’t appear
until the 4th shell
“The Shell Game”
n = 4
Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
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Completely describe the position and energy of the electron
(part of the wave function )
1. Principle quantum number (n):
n = 1, 2, 3……
gives principle energy level or
"shell"
http://www.calstatela.edu/faculty/acolvil/mineral/atom_structure2.jpg
2nn
constantsE
(just like Bohr's theory)
2. angular momentum quantum number (l) :
l = 0, 1, 2, 3……n-1
describes the type of orbital or shape
l = 0 s-orbital
l = 1 p-orbital
l = 2 d-orbital
l = 3 f-orbital
Equal to the number of
"angular nodes"
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3. magnetic quantum number (ml):
ml = - l to + l in steps of 1 (including 0)
indicates spatial orientation
If l = 0, then ml = 0 (only one kind of s-orbital)
ifl= 1, then ml = -1, 0, +1 (three kinds of p-orbitals)
if l = 2, then ml = -2, -1, 0, +1, +2 (five kinds of d-orbitals)
if l = 3, then ml = -3, -2, -1, 0, +1, +2, +3 (seven kinds of f-orbitals)
Electron Spin
• Not all spectra features explained by wave
equations:
– Appearance of “doublets” in atoms with a single
electron in outermost shell.
• Electron Spin
– Up / down.
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4. spin quantum number (ms): ms = 1/2 or -1/2
Electrons “spin” on their axis, producing a magnetic field
ms = +1/2
spin “up”
ms = -1/2
spin “down”
n = 1
2
34
5
6
l = 0 1 2 3
ml = 0
-1 0 +1
-2 -1 0 +1 +2
-3 -2 -1 0 +1 +2 +3
orbital = s p d f
max electrons/subshell = 2(2l + 1)
max electrons/shell = 2n2
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Sample Exercise 3.9:Identifying Valid Sets of Quantum Numbers
Which of these five combinations of quantum numbers are valid?
n l ml ms
(a) 1 0 -1 +1/2
(b) 3 2 -2 +1/2
(c) 2 2 0 0
(d) 2 0 0 -1/2
(e) -3 -2 -1 -1/2
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Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
Electron Configurations: In what order do electrons occupy available orbitals?
Orbital Energy Levels for Hydrogen Atoms
E
3s 3p 3d
2s 2p
1s
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Energy of orbitals in multi-electron atoms
Energy depends on n + l
1 + 0 = 1
2 + 0 = 2
2 + 1 = 3
3 + 0 = 3
3 + 1 = 4
4 + 0 = 4
3 + 2 = 5
http://www.pha.jhu.edu/~rt19/hydro/img73.gif
1s
2s
3s4s
2p
3p
4p
3d 4f4d
distance from nucleus →
"Penetration"
s > p > d > f
for the same shell (e.g.
n=4) the s-electron
penetrates closer to
the nucleus and feels a
stronger nuclear pull or
charge.
Pro
ba
bil
ity o
f fi
nd
ing
th
e e
lec
tro
n →
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Filling order of orbitals in multi-electron atoms
1s < 2s < 2p < 3s < 3p < 4s < 3d < 4p < 5s < 4d < 5p < 6s
Aufbau Principle - the lowest energy orbitals fill up first
Shorthand description of orbital occupancy
1. No more than 2 electrons maximum per orbital
2. Electrons occupy orbitals in such a way to minimize the
total energy of the atom = “Aufbau Principle”
(use filling order diagram)
3. No 2 electrons can have the same 4 quantum numbers
= “Pauli Exclusion Principle” (pair electron spins)
ms = +1/2
spin “up”
ms = -1/2
spin
“down”
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•No two electrons in an atom can have the same set of four
quantum numbers (n, l, ml, ms)
•electrons must "pair up" before entering the same orbital
4. When filling a subshell, electrons occupy empty
orbitals first before pairing up = “Hund’s Rule”
Px Py Pz
NOT
Px Py Pz
“orbital box diagram”
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Electron Shells and Orbitals
• Orbitals that have the exact same energy level are called degenerate.
• Core electrons are those in the filled, inner shells in an atom and are not involved in chemical reactions.
• Valence electrons are those in the outermost shell of an atom and have the most influence on the atom’s chemical behavior.
Px Py Pz
+
H:
He:
Li:
Be:
B:
C:
N:
O:
F:
Ne:
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Transition metals are characterized by having incompletely
filled d-subshells (or form cations as such).
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Electron Configurations from the Periodic Table
n - 1
n - 2
Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
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Electron Configurations: Ions
• Formation of Ions:
– Gain/loss of valence electrons to achieve stable electron configuration (filled shell = “octet rule”).
– Cations:
– Anions:
– Isoelectronic:
Cations of Transition MetalsOuter shell “s” and “p” electrons removed 1st
Fe = [Ar]3d64s2
Cu = [Ar]3d104s1
Sn = [Kr]4d105s25p2
Cu+
Cu
Cu2+
Fe2+
Fe3+
Fe
Sn
Sn4+
Sn2+
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Sample Exercise 3.11:Determining Isoelectronic Species in Main Group Ions
a) Determine the electron configuration of each of the following ions: Mg2+, Cl-, Ca2+, and O2-
b) Which ions are isoelectronic with Ne?
Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
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Periodic Trends – trends in atomic and ionic radii, ionization energies, and electron affinities
Effective nuclear charge (Zeff) – Inner shell electrons
“SHIELD” the outer shell electrons from the nucleus
Na
Mg
Al
Si
11
12
13
14
10
10
10
10
1
2
3
4
186
160
143
132
ZeffCoreZ Radius (nm)
Zeff = Z - s (s = shielding constant)
Zeff Z – number of inner or core electrons
Across a period -
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Down a family -
Effective nuclear charge (Zeff) – Inner shell electrons
“SHIELD” the outer shell electrons from the nucleus
Na
K
Rb
Cs
11
19
37
55
10
18
36
54
1
1
1
1
186
227
247
265
ZeffCoreZ Radius (nm)
Trends in Effective Nuclear Charge (Zeff)
and the Shielding Effect
increasing Zeff
incre
asin
g S
hie
ldin
g
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Atomic, Metallic, Ionic Radii
For diatomic molecules, equal to covalent radius (one-half the distance between nuclei).
For metals, equal to metallic radius (one-half the distance between nuclei in metal lattice).
For ions, ionic radius equals one-half the distance between ions in ionic crystal lattice.
Trends in Atomic Size for the “Representative (Main Group) Elements”
Decreasing Atomic Size
Incre
asin
g A
tom
ic S
ize
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Cation is always smaller than atom from
which it is formed.
Anion is always larger than atom from
which it is formed.
Radius of Ions
Radii of Atoms and Ionsmust compare cations to cations and anions to anions
Decreasing Ionic Radius
Incre
asin
g I
onic
Radiu
s
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Sample Exercise 3.13:Ordering Atoms and Ions by Size
Arrange each by size from largest to smallest:
(a) O, P, S
(b) Na+, Na, K
Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
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https://tinyurl.com/y8bqsr7g
Ionization energy is the minimum energy (kJ/mol)
required to remove an electron from a gaseous
atom in its ground state.
I1 + X (g) X+(g) + e-
I2 + X+(g) X2+
(g) + e-
I3 + X2+(g) X3+
g) + e-
I1 first ionization energy
I2 second ionization energy
I3 third ionization energy
I1 < I2 < I3 < …..
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General Trend in First Ionization Energies
Increasing First Ionization Energy
Decre
asin
g F
irst Io
niz
ation E
nerg
y
Ionization Energies
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Trends in the 1st Ionization Energy for the 2nd Row
Li 520 kJ/mol 1s22s1 1s2
Be 899 1s22s2 1s22s1
B 801 1s22s22p1 1s22s2
C 1086 1s22s22p2 1s22s22p1
N 1402 1s22s22p3 1s22s22p2
O 1314 1s22s22p4 1s22s22p3
F 1681 1s22s22p5 1s22s22p4
Ne 2081 1s22s22p6 1s22s22p5
Sample Exercise 3.14:Recognizing Trends in Ionization Energies
Arrange Ar, Mg, and P in order of increasing IE
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Chapter Outline
3.1 Waves of Light3.2 Atomic Spectra3.3 Particles of Light: Quantum Theory3.4 The Hydrogen Spectrum and the Bohr Model3.5 Electrons as Waves3.6 Quantum Numbers 3.7 The Sizes and Shapes of Atomic Orbitals3.8 The Periodic Table and Filling Orbitals 3.9 Electron Configurations of Ions3.10 The Sizes of Atoms and Ions3.11 Ionization Energies3.12 Electron Affinities
Electron affinity is the energy release that occurs
when an electron is accepted by an atom in the gaseous
state to form an anion.
F (g) + e- → F-(g) EA = -328 kJ/mol
O (g) + e- → O-(g) EA = -141 kJ/mol
X (g) + e- → X-(g) Energy released = E.A. (kJ/mol)