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Chapter 7 The QuantumMechanical Model of the Atom

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Title: Chapter 7 The QuantumMechanical Model of the Atom


1
Chapter 7The Quantum-Mechanical Model of the Atom
Chemistry A Molecular Approach, 1st Ed.Nivaldo
Tro
Roy Kennedy Massachusetts Bay Community
College Wellesley Hills, MA
2007, Prentice Hall
2
The Behavior of the Very Small
  • electrons are incredibly small
  • a single speck of dust has more electrons than
    the number of people who have ever lived on earth
  • electron behavior determines much of the behavior
    of atoms
  • directly observing electrons in the atom is
    impossible, the electron is so small that
    observing it changes its behavior

3
A Theory that Explains Electron Behavior
  • the quantum-mechanical model explains the manner
    electrons exist and behave in atoms
  • helps us understand and predict the properties of
    atoms that are directly related to the behavior
    of the electrons
  • why some elements are metals while others are
    nonmetals
  • why some elements gain 1 electron when forming an
    anion, while others gain 2
  • why some elements are very reactive while others
    are practically inert
  • and other Periodic patterns we see in the
    properties of the elements

4
The Nature of Lightits Wave Nature
  • light is a form of electromagnetic radiation
  • composed of perpendicular oscillating waves, one
    for the electric field and one for the magnetic
    field
  • an electric field is a region where an
    electrically charged particle experiences a force
  • a magnetic field is a region where an magnetized
    particle experiences a force
  • all electromagnetic waves move through space at
    the same, constant speed
  • 3.00 x 108 m/s in a vacuum the speed of light, c

5
Speed of Energy Transmission
6
Electromagnetic Radiation
7
Characterizing Waves
  • the amplitude is the height of the wave
  • the distance from node to crest
  • or node to trough
  • the amplitude is a measure of how intense the
    light is the larger the amplitude, the brighter
    the light
  • the wavelength, (l) is a measure of the distance
    covered by the wave
  • the distance from one crest to the next
  • or the distance from one trough to the next, or
    the distance between alternate nodes

8
Wave Characteristics
9
Characterizing Waves
  • the frequency, (n) is the number of waves that
    pass a point in a given period of time
  • the number of waves number of cycles
  • units are hertz, (Hz) or cycles/s s-1
  • 1 Hz 1 s-1
  • the total energy is proportional to the amplitude
    and frequency of the waves
  • the larger the wave amplitude, the more force it
    has
  • the more frequently the waves strike, the more
    total force there is

10
The Relationship Between Wavelength and Frequency
  • for waves traveling at the same speed, the
    shorter the wavelength, the more frequently they
    pass
  • this means that the wavelength and frequency of
    electromagnetic waves are inversely proportional
  • since the speed of light is constant, if we know
    wavelength we can find the frequency, and visa
    versa

11
Example 7.1- Calculate the wavelength of red
light with a frequency of 4.62 x 1014 s-1
n 4.62 x 1014 s-1 l, (nm)
Given Find
ln c, 1 nm 10-9 m
Concept Plan Relationships
Solve
the unit is correct, the wavelength is
appropriate for red light
Check
12
Practice Calculate the wavelength of a radio
signal with a frequency of 100.7 MHz
13
Practice Calculate the wavelength of a radio
signal with a frequency of 100.7 MHz
n 100.7 MHz l, (m)
Given Find
Concept Plan Relationships
ln c, 1 MHz 106 s-1
Solve
the unit is correct, the wavelength is
appropriate for radiowaves
Check
14
Color
  • the color of light is determined by its
    wavelength
  • or frequency
  • white light is a mixture of all the colors of
    visible light
  • a spectrum
  • RedOrangeYellowGreenBlueViolet
  • when an object absorbs some of the wavelengths of
    white light while reflecting others, it appears
    colored
  • the observed color is predominantly the colors
    reflected

15
Amplitude Wavelength
16
Electromagnetic Spectrum
17
Continuous Spectrum
18
The Electromagnetic Spectrum
  • visible light comprises only a small fraction of
    all the wavelengths of light called the
    electromagnetic spectrum
  • short wavelength (high frequency) light has high
    energy
  • radiowave light has the lowest energy
  • gamma ray light has the highest energy
  • high energy electromagnetic radiation can
    potentially damage biological molecules
  • ionizing radiation

19
Thermal Imaging using Infrared Light
20
Using High Energy Radiationto Kill Cancer Cells
21
Interference
  • the interaction between waves is called
    interference
  • when waves interact so that they add to make a
    larger wave it is called constructive
    interference
  • waves are in-phase
  • when waves interact so they cancel each other it
    is called destructive interference
  • waves are out-of-phase

22
Interference
23
Diffraction
  • when traveling waves encounter an obstacle or
    opening in a barrier that is about the same size
    as the wavelength, they bend around it this is
    called diffraction
  • traveling particles do not diffract
  • the diffraction of light through two slits
    separated by a distance comparable to the
    wavelength results in an interference pattern of
    the diffracted waves
  • an interference pattern is a characteristic of
    all light waves

24
Diffraction
25
2-Slit Interference
26
The Photoelectric Effect
  • it was observed that many metals emit electrons
    when a light shines on their surface
  • this is called the Photoelectric Effect
  • classic wave theory attributed this effect to the
    light energy being transferred to the electron
  • according to this theory, if the wavelength of
    light is made shorter, or the light waves
    intensity made brighter, more electrons should be
    ejected
  • remember the energy of a wave is directly
    proportional to its amplitude and its frequency
  • if a dim light was used there would be a lag time
    before electrons were emitted
  • to give the electrons time to absorb enough energy

27
The Photoelectric Effect
28
The Photoelectric EffectThe Problem
  • in experiments with the photoelectric effect, it
    was observed that there was a maximum wavelength
    for electrons to be emitted
  • called the threshold frequency
  • regardless of the intensity
  • it was also observed that high frequency light
    with a dim source caused electron emission
    without any lag time

29
Einsteins Explanation
  • Einstein proposed that the light energy was
    delivered to the atoms in packets, called quanta
    or photons
  • the energy of a photon of light was directly
    proportional to its frequency
  • inversely proportional to it wavelength
  • the proportionality constant is called Plancks
    Constant, (h) and has the value 6.626 x 10-34 Js

30
Example 7.2- Calculate the number of photons in a
laser pulse with wavelength 337 nm and total
energy 3.83 mJ
l 337 nm, Epulse 3.83 mJ number of photons
Given Find
Ehc/l, 1 nm 10-9 m, 1 mJ 10-3 J,
Epulse/Ephoton photons
Concept Plan Relationships
Solve
31
Practice What is the frequency of radiation
required to supply 1.0 x 102 J of energy from
8.5 x 1027 photons?
32
What is the frequency of radiation required to
supply 1.0 x 102 J of energy from 8.5 x 1027
photons?
Etotal 1.0 x 102 J, number of photons 8.5 x
1027 n
Given Find
Ehn, Etotal Ephoton photons
Concept Plan Relationships
Solve
33
Ejected Electrons
  • 1 photon at the threshold frequency has just
    enough energy for an electron to escape the atom
  • binding energy, f
  • for higher frequencies, the electron absorbs more
    energy than is necessary to escape
  • this excess energy becomes kinetic energy of the
    ejected electron
  • Kinetic Energy Ephoton Ebinding
  • KE hn - f

34
Spectra
  • when atoms or molecules absorb energy, that
    energy is often released as light energy
  • fireworks, neon lights, etc.
  • when that light is passed through a prism, a
    pattern is seen that is unique to that type of
    atom or molecule the pattern is called an
    emission spectrum
  • non-continuous
  • can be used to identify the material
  • flame tests
  • Rydberg analyzed the spectrum of hydrogen and
    found that it could be described with an equation
    that involved an inverse square of integers

35
Emission Spectra
36
Exciting Gas Atoms to Emit Light with Electrical
Energy
37
Examples of Spectra
38
Identifying Elements with Flame Tests
39
Emission vs. Absorption Spectra
Spectra of Mercury
40
Bohrs Model
  • Neils Bohr proposed that the electrons could only
    have very specific amounts of energy
  • fixed amounts quantized
  • the electrons traveled in orbits that were a
    fixed distance from the nucleus
  • stationary states
  • therefore the energy of the electron was
    proportional the distance the orbital was from
    the nucleus
  • electrons emitted radiation when they jumped
    from an orbit with higher energy down to an orbit
    with lower energy
  • the distance between the orbits determined the
    energy of the photon of light produced

41
Bohr Model of H Atoms
42
Wave Behavior of Electrons
  • de Broglie proposed that particles could have
    wave-like character
  • because it is so small, the wave character of
    electrons is significant
  • electron beams shot at slits show an interference
    pattern
  • the electron interferes with its own wave
  • de Broglie predicted that the wavelength of a
    particle was inversely proportional to its
    momentum

43
Electron Diffraction
44
Example 7.3- Calculate the wavelength of an
electron traveling at 2.65 x 106 m/s
v 2.65 x 106 m/s, m 9.11 x 10-31 kg (back
leaf) l, m
Given Find
lh/mv
Concept Plan Relationships
Solve
45
Practice - Determine the wavelength of a neutron
traveling at 1.00 x 102 m/s(Massneutron 1.675
x 10-24 g)
46
Practice - Determine the wavelength of a neutron
traveling at 1.00 x 102 m/s
v 1.00 x 102 m/s, m 1.675 x 10-24 g l, m
Given Find
lh/mv, 1 kg 103 g
Concept Plan Relationships
Solve
47
Complimentary Properties
  • when you try to observe the wave nature of the
    electron, you cannot observe its particle nature
    and visa versa
  • wave nature interference pattern
  • particle nature position, which slit it is
    passing through
  • the wave and particle nature of nature of the
    electron are complimentary properties
  • as you know more about one you know less about
    the other

48
Uncertainty Principle
  • Heisenberg stated that the product of the
    uncertainties in both the position and speed of a
    particle was inversely proportional to its mass
  • x position, Dx uncertainty in position
  • v velocity, Dv uncertainty in velocity
  • m mass
  • the means that the more accurately you know the
    position of a small particle, like an electron,
    the less you know about its speed
  • and visa-versa

49
Uncertainty Principle Demonstration
any experiment designed to observe the electron
results in detection of a single electron
particle and no interference pattern
50
Determinacy vs. Indeterminacy
  • according to classical physics, particles move in
    a path determined by the particles velocity,
    position, and forces acting on it
  • determinacy definite, predictable future
  • because we cannot know both the position and
    velocity of an electron, we cannot predict the
    path it will follow
  • indeterminacy indefinite future, can only
    predict probability
  • the best we can do is to describe the probability
    an electron will be found in a particular region
    using statistical functions

51
Trajectory vs. Probability
52
Electron Energy
  • electron energy and position are complimentary
  • because KE ½mv2
  • for an electron with a given energy, the best we
    can do is describe a region in the atom of high
    probability of finding it called an orbital
  • a probability distribution map of a region where
    the electron is likely to be found
  • distance vs. y2
  • many of the properties of atoms are related to
    the energies of the electrons

53
Wave Function, y
  • calculations show that the size, shape and
    orientation in space of an orbital are determined
    be three integer terms in the wave function
  • added to quantize the energy of the electron
  • these integers are called quantum numbers
  • principal quantum number, n
  • angular momentum quantum number, l
  • magnetic quantum number, ml

54
Principal Quantum Number, n
  • characterizes the energy of the electron in a
    particular orbital
  • corresponds to Bohrs energy level
  • n can be any integer ³ 1
  • the larger the value of n, the more energy the
    orbital has
  • energies are defined as being negative
  • an electron would have E 0 when it just escapes
    the atom
  • the larger the value of n, the larger the orbital
  • as n gets larger, the amount of energy between
    orbitals gets smaller

55
Principal Energy Levels in Hydrogen
56
Electron Transitions
  • in order to transition to a higher energy state,
    the electron must gain the correct amount of
    energy corresponding to the difference in energy
    between the final and initial states
  • electrons in high energy states are unstable and
    tend to lose energy and transition to lower
    energy states
  • energy released as a photon of light
  • each line in the emission spectrum corresponds to
    the difference in energy between two energy states

57
Predicting the Spectrum of Hydrogen
  • the wavelengths of lines in the emission spectrum
    of hydrogen can be predicted by calculating the
    difference in energy between any two states
  • for an electron in energy state n, there are (n
    1) energy states it can transition to, therefore
    (n 1) lines it can generate
  • both the Bohr and Quantum Mechanical Models can
    predict these lines very accurately

58
Hydrogen Energy Transitions
59
Example 7.7- Calculate the wavelength of light
emitted when the hydrogen electron transitions
from n 6 to n 5
ni 6, nf 5 l, m
Given Find
Ehc/l, En -2.18 x 10-18 J (1/n2)
Concept Plan Relationships
DEatom -Ephoton
Solve
Ephoton -(-2.6644 x 10-20 J) 2.6644 x 10-20 J
Check
the unit is correct, the wavelength is in the
infrared, which is appropriate because less
energy than 4?2 (in the visible)
60
Practice Calculate the wavelength of light
emitted when the hydrogen electron transitions
from n 2 to n 1
61
Calculate the wavelength of light emitted when
the hydrogen electron transitions from n 2 to n
1
ni 2, nf 1 l, m
Given Find
Ehc/l, En -2.18 x 10-18 J (1/n2)
Concept Plan Relationships
DEatom -Ephoton
Solve
Ephoton -(-1.64 x 10-18 J) 1.64 x 10-18 J
Check
the unit is correct, the wavelength is in the UV,
which is appropriate because more energy than 3?2
(in the visible)
62
Probability Radial Distribution Functions
  • y2 is the probability density
  • the probability of finding an electron at a
    particular point in space
  • for s orbital maximum at the nucleus?
  • decreases as you move away from the nucleus
  • the Radial Distribution function represents the
    total probability at a certain distance from the
    nucleus
  • maximum at most probable radius
  • nodes in the functions are where the probability
    drops to 0

63
Probability Density Function
64
Radial Distribution Function
65
The Shapes of Atomic Orbitals
  • the l quantum number primarily determines the
    shape of the orbital
  • l can have integer values from 0 to (n 1)
  • each value of l is called by a particular letter
    that designates the shape of the orbital
  • s orbitals are spherical
  • p orbitals are like two balloons tied at the
    knots
  • d orbitals are mainly like 4 balloons tied at the
    knot
  • f orbitals are mainly like 8 balloons tied at the
    knot

66
l 0, the s orbital
  • each principal energy state has 1 s orbital
  • lowest energy orbital in a principal energy state
  • spherical
  • number of nodes (n 1)

67
2s and 3s
2s n 2, l 0
3s n 3, l 0
68
l 1, p orbitals
  • each principal energy state above n 1 has 3 p
    orbitals
  • ml -1, 0, 1
  • each of the 3 orbitals point along a different
    axis
  • px, py, pz
  • 2nd lowest energy orbitals in a principal energy
    state
  • two-lobed
  • node at the nucleus, total of n nodes

69
p orbitals
70
l 2, d orbitals
  • each principal energy state above n 2 has 5 d
    orbitals
  • ml -2, -1, 0, 1, 2
  • 4 of the 5 orbitals are aligned in a different
    plane
  • the fifth is aligned with the z axis, dz squared
  • dxy, dyz, dxz, dx squared y squared
  • 3rd lowest energy orbitals in a principal energy
    state
  • mainly 4-lobed
  • one is two-lobed with a toroid
  • planar nodes
  • higher principal levels also have spherical nodes

71
d orbitals
72
l 3, f orbitals
  • each principal energy state above n 3 has 7 d
    orbitals
  • ml -3, -2, -1, 0, 1, 2, 3
  • 4th lowest energy orbitals in a principal energy
    state
  • mainly 8-lobed
  • some 2-lobed with a toroid
  • planar nodes
  • higher principal levels also have spherical nodes

73
f orbitals
74
Why are Atoms Spherical?
75
Energy Shells and Subshells
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