chapter 12 handouts
TRANSCRIPT
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Chapter 2: Quantum Mechanics and Atomic Theory
Chapter 12: Phenomena
Phenomena: Different wavelengths of electromagnetic radiation were directedonto two different metal sample (see picture). Scientist then record if anyparticles were ejected and if so what type of particle as well as the speed of theparticle. What patterns do you see in the results that were collected?
KExp.
Wavelength of LightDirected atSample
IntensityWhere Particles
EjectedEjectedParticle
Speed ofEjected Particle
1 5.410-7 m Medium Yes e- 4.9104
2 3.310-8 m High Yes e- 3.5106
3 2.0 m High No N/A N/A
4 3.310-8 m Low Yes e- 3.5106
5 2.0 m Medium No N/A N/A
6 6.110-12 m High Yes e- 2.7108
7 5.5104 m High No N/A N/A
FeExp.
Wavelength of LightDirected atSample
Where ParticlesEjected
EjectedParticle
Speed ofEjected Particle
1 5.410-7 m Medium No N/A N/A
2 3.410-11 m High Yes e- 1.1108
3 3.9103 m Medium No N/A N/A
4 2.410-8 m High Yes e- 4.1106
5 3.9103 m Low No N/A N/A
6 2.610-7 m Low Yes e- 1.1105
7 3.410-11 m Low Yes e- 1.1108
EjectedParticle
ElectromagneticRadiation
Chapter 12:QuantumMechanics andAtomic Theory
o Electromagnetic
Radiation
o Quantum Theory
o Particle in a Box
o The Hydrogen Atom
o Quantum Numbers
o Orbitals
o Many Electron Atoms
o Periodic Trends
2
Big Idea: The structure of atomsmust be explainedusing quantummechanics, a theory in
which the properties of
particles and wavesmerge together.
Chapter 2: Quantum Mechanics and Atomic Theory
Electromagnetic Radiation
Electromagnetic Radiation:Consists of oscillating(time-varying)electric and magnetic fields thattravel through space at 2.998 108
(c = speed
of light) or just over 660 million mph.
3
Note All forms of radiation transfer energy from one region of space into another.
Examples of Electromagnetic Radiation
Visible light
Radio Waves
X-Rays
Chapter 2: Quantum Mechanics and Atomic Theory
Electromagnetic Radiation
Wavelength (): Is thepeak-to-peak distance.
Amplitude: Determinesbrightness of theradiation.
Frequency (): Thenumber of cycles persecond (1 1
).
4
Note
Changing the wavelength changes the
region of the spectrum (i.e. x-ray to visible).
Chapter 2: Quantum Mechanics and Atomic Theory
Electromagnetic Radiation
5Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
If white light is passedthrough a prism, acontinuous spectrumof light is found.However, when the
light emitted byexcited hydrogenatoms is passedthrough a prism theradiation is found toconsist of a numberof components orspectra lines.
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Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Black Body: An object that absorbs and emits allfrequencies of radiation without favor.
Heated Black Bodies
. .
7
Note max is the most prevalent wavelength, not the longest wavelength.
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Theory
Scientists used classical physics arguments toderive an expression for the energy density
(Rayleigh Jens Law).
The Problem With Explaining Black Body RadiationUsing Classical Mechanics
Classical mechanics put
no limits on minimum
wavelength therefore at
very small , would be a
huge value even for low temperatures.
8
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Max Plank: Proposed that the exchangeof energy between matter and radiationoccurs in quanta, or packets of energy.His central idea was that a chargedparticle oscillating at a frequency , canexchange energy with its surroundings bygenerating or absorbing electromagneticradiation only in discrete packets ofenergy.
9
Quanta: Packet of energy (implies minimumenergy that can be emitted).
Charged particles oscillating at a frequency, ,can only exchange energy with theirsurroundings in discrete packets of energy.
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Photoelectric Effect:Ejection of electrons from ametal when its surface is exposed to ultra violetradiation.
10
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Findings of the Photoelectric Effect
1) No electrons are ejected unless the radiation has afrequency above a certain threshold valuecharacteristic of the metal.
2) Electrons are ejected immediately, however low theintensity of the radiation.
3) The kinetic energy of the ejected electronsincreases linearly with the frequency of the incidentradiation.
Albert Einstein
Proposed that electromagnetic radiation consistsof massless particles (photons)
Photons are packets of energy
Energy of a single photon =
11Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Photoelectric Effect Electromagnetic radiation consists of streams of photons
traveling with frequency, , and energy .
Photons collide with metal.
If the photons have enough energy, electrons will be
removed from the metal.
Work Function ():The minimum amount ofenergy required to remove an electron from thesurface of a metal.
If no electron ejected
If electron will be ejected
12
Note This relationship is not intensity dependent.
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Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
With what speed will the fastest electronsbe emitted from a surface whose
threshold wavelength is 600. nm, whenthe surface is illuminated with l ight ofwavelength 4.010
7?
13Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
H atoms only emit/absorb certainfrequencies.
What is causing these properties?
Electrons can only exist withcertain energies.
The spectral lines are transitionsfrom one allowed energy level toanother.
14
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Finding energy levels of H atom
3.29 10
(Found experimentally)
3.29 10
6.626 10
3.29 10
-2.178 10
=
Energ y leve l of H ato m
2.178 10
n= 1, 2, 3,
Energ y level of othe r 1e-system s
2.178 10
n= 1, 2, 3,
15
Note In this equation n2 is always the large number which corresponds to the
higher energy level.
Note
The negative sign appeared because a negative sign was taken out of
parenthesis.
Chapter 2: Quantum Mechanics and Atomic Theory
Student Question
Quantum Theory
What is the wavelength of the radiationemitted by a 2
atom when an electron
transitions between 4 to the 2 levels?
Help ful Hint: c = 2.998108
a ) -1.6641024m
b ) -5.39910-8m
c ) 1.62110-7m
d ) 4.86410-7m
e )None o f t he Above
16
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
ConstructiveInterference: When thepeaks of wavescoincide, the amplitudeof the resulting wave is
increased.
Destructive Interference:When the peak of onewave coincides with thetrough of another wavethe resulting wave isdecreased.
17Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
When light passes
though a pair of closely
spaced slits, circularwaves are generated at
each slit. These waves
interfere with each
other.
Where they interfereconstructively, a bright
line is seen on the screen
behind the slits; where
the interference is
destructive, the screen is
dark.
18
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Chapter 2: Quantum Mechanics and Atomic Theory
Student Question
Quantum Theory
What is the wavelength of an electron travelingat
the speed of light?
Helpful informa t ion: 9.109 10 a n dh = 6.62610-34Js
a ) 2.4210-9m
b ) 2.4210-12m
c ) 4.121011m
d )None o f t he Above
19Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Particles have wave like properties, therefore,classical mechanics are incorrect.
Classical Mechanics:
Particles have a defined trajectory.
Location and linear momentum can bespecified at every moment.
Quantum Mechanics:
Particles behave like waves.
Cannot specify the precise location of aparticle.
20
Note For the hydrogen atom, the duality means that we are not going to be able
to know the speed of an electron orbiting the nucleus in a definite trajectory.
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Theory
Wavefunction ():A solution of the Schrdingerequation; the probability amplitude.
Probability Density ():A function that, whenmultiplied by volume of the region, gives theprobability that the particle will be found in thatregion of space.
21
Note This gives you a representation of the particles trajectory.
Examples
sin
Note This value must be between 0 and 1
Chapter 2: Quantum Mechanics and Atomic Theory
Particle in a Box
Particle in a 1-D Box
Boundary Conditions
0 0
0
What is the wavefunction?
sin sin0 0 sin 0
22
Note The term
is there for normalization in order to get 1
Note n is a quantum number. Quantum numbers are integers or integers
that label a wavefunction.
Chapter 2: Quantum Mechanics and Atomic Theory
Take 1st derivative of
Take 2nd derivative of
Particle in a Box
Get the allowed energy levels from Schrdingers equation
23
What are the allowed energy levels?
Note V(x)=0 for the particle in a box
Chapter 2: Quantum Mechanics and Atomic Theory
Particle in a Box
Plug 2nd derivative back into wavefunction
sin
sin
Cancel out
Simplify
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Chapter 2: Quantum Mechanics and Atomic Theory
The Hydrogen Atom
Atomic Orbitals:A regionof space in which there isa high probability offinding an electron in an
atom.
The wavefunction of an electron is given inspherical polar coordinates
= distance from the center of the atom
= the angle from the positive z-axis, which can bethought of as playing the role of the geographicallatitude
= the angle about the z-axis, the geographicallongitude
25
Note The wavefunctions of electrons
are the atomic orbitals.
Chapter 2: Quantum Mechanics and Atomic Theory
The Hydrogen Atom
Wavefunction of an electron in a1-electron atom
,, ,
Radial Wavefunction
, Angular Wavefunction
26
Chapter 2: Quantum Mechanics and Atomic Theory
The Hydrogen Atom
General wavefunction expression for a hydrogenatom:
27
+1
-1
0
+2
-1
+1
-2
0
Chapter 2: Quantum Mechanics and Atomic Theory
The Hydrogen Atom
Schrdinger Equation for the H-atom
sin
Columbic potential energy between the protonand electron
Reduced mass (proton and electron)
Scientists have solved for the energy of the H-atom
.
3.290 10
principle quantum number can be 1, 2, 3,
planks constant 6.6260810-34Js
28
Chapter 2: Quantum Mechanics and Atomic Theory
The Hydrogen Atom
Pictured: Thepermitted energylevels of ahydrogen atom.
The levels arelabeled with thequantum number which rangesfrom 1 (groundstate) to .
29Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Numbers
Principle Quantum Number
Rela ted To: Size and Energy
Al low ed Values: 1,2,3, (shells)
30
Note The larger the , the larger the size, the larger the orbital, and the larger theenergy.
Note When identifying the orbital, the value comes in front of the orbital type.
Example
3p 3
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Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Numbers
Angular MomentumQuantum Number ()
Relate d To:Shape
Al low ed Values: 0,1,2, , 1 (subshells)
What are the possible valuesgiven the following values?
1 1
2 2
3 3
What type of orbital is associated withthe following quantum numbers?
1 1 and 0
2 2 and 13 3 and 0
31
Valueof l
OrbitalType
0 s
1 p
2 d
3 f
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Numbers
Magnetic Quantum Number ()
Rela te d To: Orientation in space
(specifies exactly which orbital [ex: ])Al low ed Va lues: , 1, ,0 , , (orbitals)
What are the possible values of given thefollowing and values:
1 1 and 0
2 2 and 1
3 2 and 0
32
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Numbers
33
Note The quantum number ml is an alternative label for the individual orbitals: inchemistry, it is more common to use x, y, and z instead.
Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Numbers
A summary of the arrangements of shells,subshells, and orbitals in an atom and the
corresponding quantum numbers.
34
Chapter 2: Quantum Mechanics and Atomic Theory
Student Question
Quantum Numbers
The following set of quantum numbers is notallowed: 3, 0, 2. Assuming thatthe and values are correct, change the value to an allowable combination.
a) 1
b) 2
c) 3
d) 4
e) None of the Above
35Chapter 2: Quantum Mechanics and Atomic Theory
Quantum Numbers
Electron Spin Quantum Number()
Rela te d To:Spin of the electron
Al low ed Va lues: (spin up ) or - (spindown )
36
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Chapter 2: Quantum Mechanics and Atomic Theory
Orbitals
What does an s-orbital ( 0) look like?
1 and 0
(radial wavefunction)
,
(angular wavefuction)
, ,
, ,
37Chapter 2: Quantum Mechanics and Atomic Theory
Orbitals
The three s-orbitals ( ) of lowest energy
The simplest way ofdrawing an atomic
orbital is as a boundarysurface, a surface within which there is a high probability
(typically 90%) of finding the electron. The darker theshaded region within the boundary surfaces, the larger the
probability of the electron being found there.
38
Chapter 2: Quantum Mechanics and Atomic Theory
Orbitals
What do p-orbitals ( 1) look like?
39Chapter 2: Quantum Mechanics and Atomic Theory
Orbitals
What do d-orbitals ( 2) look like?
40
Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
The electrons in many-electron atomsoccupy orbitals like those of hydrogenbut the energy of the orbitals differ.
Differences between the many-electronorbital energies and hydrogen atomorbital energies:
The nucleus of the many-electron orbitals havemore positive charge attracting the electrons,thus lowering the energy.
The electrons repel each other raising theenergy.
41Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
The number of electrons in an atom affects theproperties of the atom.
42
Note H with 1 electron has no electron-electron repulsion and the electron will have
the same energy if is the 2s or 2p orbital (all orbitals within one shell degenerate).
Potential Energy for He atom (2 p and 2 e-)
Attraction of
electron 1 to
the nucleus
Attraction of
electron 2 to
the nucleus
Repulsion
between the
two electrons
2
4
2
4
4
1 = distance between electron 1 and the nucleus
2 = distance between electron 2 and the nucleus
12 = distance between the two electrons
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Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
Why do the energies change?
Shielding: The repulsion experienced byan electron in an atom that arises from
the other electrons present andopposes the attraction exerted by thenucleus.
Effective Nuclear Charge (Zeff):The netnuclear charge after taking intoaccount the shielding caused by otherelectrons in the atom.
43
Amount of Shielding
Distance from nucleus
Note s electrons can penetrate through the nucleus while p and
d electrons cannot.
S P D F
Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
44
Order of Orbital Filling
1s 2s 2p 3s 3p 4s 3d 4p 5s 4d 5p
7s 7p 7d 7f
6s 6p 6d 6f
5s 5p 5d 5f
4s 4p 4d 4f
3s 3p 3d
2s 2p
1s
Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
Electron Configuration: A list of an atomsoccupied orbitals with the number of electronsthat each contains.
In the ground state the electrons occupy atomic orbitals
in such a way that the total energy of the atom is aminimum.
We might expect that atoms would have all their
electrons in the 1s orbital however this is only true for Hand He.
Pauli Exclusion Principle: No more than twoelectrons may occupy any given orbital. Whentwo electrons occupy one orbital, the spins mustbe paired.
45
Note Paired spins means and electron ()
Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
Writing Electron Configurations
Step 1:Determine the number of electrons theatom has.
Step 2: Fill atomic orbitals starting with lowestenergy orbitals first and proceeding to higherenergy orbitals.
Step 3:Determine how electrons fill the orbitals.
46
Subshell lSmallest
ns 0 1p 1 2d 2 3f 3 4
Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
Electron Configurations: He Step 1:
Step 2:
Step 3:
Be Step 1:
Step 2:
Step 3:
47Chapter 2: Quantum Mechanics and Atomic Theory
Many Electron Atoms
Electron Configurations: C Step 1:
Step 2:
Step 3: __ __ __ 2p __ __ __ 2p __ __ __ 2p
2s 2s 2s
1s 1s 1s
48
Note Electrons that are farther apart repel each other less.
Note Electrons with parallel spins tend to avoid each other more.
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Chapter 2: Quantum Mechanics and Atomic Theory
Periodic Trends
Effective NuclearCharge:(Zeff) The netnuclear charge aftertaking into accountthe shielding causedby other electrons inthe atom.
Why:Going across the periodic table, the numberof core electrons stays the same but the number
of protons increases. The core electrons are
responsible for most of the shielding, therefore the
Zeff gets larger as you go across a period.
Although going down a group adds more coreelectrons it also adds more protons therefore Zeff is
pretty much constant going down a group.
49Chapter 2: Quantum Mechanics and Atomic Theory
Periodic Trends
Atomic Radii:Half the distancebetween the centers
of neighboring atomsin a solid of ahomonuclearmolecule.
Why:Going across a period the Zeff increases,therefore the pull on the electrons increases andthe atomic radii decrease. Going down a group,
more atomic shells are added and the radii
increase.
50
Chapter 2: Quantum Mechanics and Atomic Theory
Periodic Trends
First Ionization Energy:The minimum energyrequired to remove thefirst electron from theground state of agaseous atom,molecule, or ion.
X(g) X+(g) +e-
Why:Going across a period the Zeff increasestherefore it is harder to remove an electron and
the first ionization energy increases. However,
going down a group the electrons are located
farther from the nucleus and they can be
removed easier.
51Chapter 2: Quantum Mechanics and Atomic Theory
Periodic Trends
1st Ionization Energy Data
Why dont B and Al fit the 1st ionization energy trend?
52
H
He
Li
BeB
C
NO
F
Ne
Na
MgAl
Si
P S
Cl
Ar
KCa
0
500
1000
1500
2000
2500
0 1 2 3 4 5 6 7 8 9 1 0 11 12 13 14 15 16 17 18 19 20
Ionizationenergy,kJmol-1
Atomic Number
Ionization Energies of the First 20 Elements
Chapter 2: Quantum Mechanics and Atomic Theory
Periodic Trends
Electron Affinity: (Eea)The energy releasedwhen an electron isadded to agas-phase atom.
X(g) + e- X-(g)
Why:Going across a period the Zeff increasestherefore the atom has a larger positive charge
and releases more energy when an electron is
added to the atom. Going down a group theelectron is added farther from the nucleus and the
electron affinity decreases. This trend does not holdtrue for the noble gases.
53
Note This trends has the most atoms that do not obey it.
Chapter 2: Quantum Mechanics and Atomic Theory
Periodic Trends
54
H
He
Li
BeB
C
N
O
F
Ne
Na
Mg
Al
Si
P
S
Cl
Ar
K
Ca
-50
0
50
100
150
200
250
300
350
400
0 1 2 3 4 5 6 7 8 9 1 0 11 12 13 14 15 16 17 18 19 20
EA(kJ/mole)
Atomic Number
Electron Affinity of the First 20 Elements
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Chapter 2: Quantum Mechanics and Atomic Theory
Take Away From Chapter 12
Big Idea: The structure of atoms must be explainedusing quantum mechanics, a theory in which theproperties of particles and waves merge together.
Electromagnetic Radiation (22)
Be able to change between frequency and wavelength
Be able to assign what area of the electromagneticspectrum radiation comes from.
55
Numbers correspond to end of chapter questions.
Chapter 2: Quantum Mechanics and Atomic Theory
Take Away From Chapter 12
Quantum Theory
Know that electromagnetic radiation has both wave andmatter properties. (30)
Photo electric effect (particle property) (27, 28, 29)
Know what the work function of a material is Diffraction (wave property)
Be able to calculate the energy carried in an
electromagnetic wave (21, 25)
Know that matter has both wave and matter properties.
Be able to calculate the wavelength of matter. (32, 34, 35)
Know that the Heisenberg uncertainty principle determines
the accuracy in which we can measure momentum andposition.
56
Numbers correspond to end of chapter questions.
Chapter 2: Quantum Mechanics and Atomic Theory
Take Away From Chapter 12
Particle in a Box
Know that the wavefunction of different systems can be
found using boundary conditions.
Particle in a box wavefunction
sin
Know that the square of the wavefunction tells us the
probability of the particle being in a certain location
Know the most likely location of a particle in a box (ex: n = 1
particle most likely in center of box, n = 2 particle most likely onsides of box)
Know that the Schrdinger equation allows us to matchwavefunctions with allowed energy values.
Particle in a box
(53, 54, 55, 57)
The Hydrogen Atom
Know that when quantum mechanics is applied to 1
electron systems the observed energy and the theoretical
energies match. (38, 40, 41, 42, 44, 46, 47, 141) 2.178 10
57
Numbers correspond to end of chapter questions.
Chapter 2: Quantum Mechanics and Atomic Theory
Take Away From Chapter 12
Quantum Number (58,62,64,65,66, 74,75) Know that the quantum number gives the size and
energy
Allowed values of 1,2,
Know that the quantum number l gives the orbital type(shape)
Allowed values of 0 ,1 ,2 , 1
Know that the quantum number gives the orbitalorientation (ex: ) Allowed values of ,0,
Know that a fourth quantum number was needed to have theory
match experiment, Allowed values of
58
Numbers correspond to end of chapter questions.
Chapter 2: Quantum Mechanics and Atomic Theory
Take Away From Chapter 12
Orbitals Know that when atomic orbitals are drawn they represent the
area in which e- have a 90% chance of being in. (67)
Know the what s, p, and d orbitals look like.
Many Electron Atoms
Be able to write both the full and shorthand electronconfigurations of atoms.(76, 77, 80, 84, 92)
Be able to predict the number of unpaired electrons in asystem.(90, 91)
Periodic Trends Know the trends of effective nuclear charge, atomic radii,
ionization energy, and electron affinity. (13, 14, 96, 97, 98, 100, 106,
111, 112, 133, 136)
59
Numbers correspond to end of chapter questions.