Title: Chapter 7 The QuantumMechanical Model of the Atom
1Chapter 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
2The 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
3A 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
4The 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
5Speed of Energy Transmission
6Electromagnetic Radiation
7Characterizing 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
8Wave Characteristics
9Characterizing 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
10The 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
11Example 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
12Practice Calculate the wavelength of a radio
signal with a frequency of 100.7 MHz
13Practice 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
14Color
- 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
15Amplitude Wavelength
16Electromagnetic Spectrum
17Continuous Spectrum
18The 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
19Thermal Imaging using Infrared Light
20Using High Energy Radiationto Kill Cancer Cells
21Interference
- 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
22Interference
23Diffraction
- 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
24Diffraction
252-Slit Interference
26The 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
27The Photoelectric Effect
28The 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
29Einsteins 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
30Example 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
31Practice What is the frequency of radiation
required to supply 1.0 x 102 J of energy from
8.5 x 1027 photons?
32What 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
33Ejected 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
34Spectra
- 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
35Emission Spectra
36Exciting Gas Atoms to Emit Light with Electrical
Energy
37Examples of Spectra
38Identifying Elements with Flame Tests
39Emission vs. Absorption Spectra
Spectra of Mercury
40Bohrs 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
41Bohr Model of H Atoms
42Wave 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
43Electron Diffraction
44Example 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
45Practice - Determine the wavelength of a neutron
traveling at 1.00 x 102 m/s(Massneutron 1.675
x 10-24 g)
46Practice - 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
47Complimentary 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
48Uncertainty 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
49Uncertainty Principle Demonstration
any experiment designed to observe the electron
results in detection of a single electron
particle and no interference pattern
50Determinacy 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
51Trajectory vs. Probability
52Electron 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
53Wave 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
54Principal 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
55Principal Energy Levels in Hydrogen
56Electron 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
57Predicting 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
58Hydrogen Energy Transitions
59Example 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)
60Practice Calculate the wavelength of light
emitted when the hydrogen electron transitions
from n 2 to n 1
61Calculate 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)
62Probability 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
63Probability Density Function
64Radial Distribution Function
65The 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
66l 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)
672s and 3s
2s n 2, l 0
3s n 3, l 0
68l 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
69p orbitals
70l 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
71d orbitals
72l 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
73f orbitals
74Why are Atoms Spherical?
75Energy Shells and Subshells