chapter 12 quantum mechanics and atomic theory 5.1 electromagnetic radiation 5.2 the nature of...
TRANSCRIPT
![Page 1: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/1.jpg)
Chapter 12Quantum Mechanics and Atomic Theory
5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr Model 5.5 The Quantum Mechanical Description of the Atom 5.6 The Particle in a Box (skip) 5.7 The Wave Equation for the Hydrogen Atom 5.8 The Physical Meaning of a Wave Function 5.9 The Characteristics of Hydrogen Orbitals 5.10 Electron Spin and the Pauli Principle 5.11 Polyelectronic Atoms 5.12 The History of the Periodic Table 5.13 The Aufbau Principle and the Periodic Table 5.14 Further Development of the Polyelectronic Model 5.15 Periodic Trends in Atomic Properties 5.16 The Properties of Alkali Metals
![Page 2: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/2.jpg)
Waves and Light
• Electromagnetic Radiation– Energy travels through space as electromagnetic
radiation– Examples: visible light, microwave radiation, radio
waves, X-rays, infra-red radiation, UV radiation– Waves (characterized by λ, υ, amp, c) – Travels at the speed of light (3x108 m/sec)
![Page 3: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/3.jpg)
Light consists of waves of oscillating electric (E) and magnetic fields (H) that are perpendicular to one another and to the direction of propagation of the light.
Electromagnetic Radiation
![Page 4: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/4.jpg)
400 nm (violet) The visible spectrum 700 nm (red)
Electromagnetic Spectrum
![Page 5: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/5.jpg)
![Page 6: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/6.jpg)
Important Equations(that apply to EM radiation)
• c = λυc=lambda nu)
c = 3 x 108 meters / second
λ = wavelength [m, nm (10-9m), Å (10-10m)]= frequency (Hz = s-1)
[frequency and wavelength vary inversely]
• E = hυ (Energy = h nu)
h = Planck’s constant
(h = 6.62 x 10-34 J s = 6.62 x 10-34 kg m2 s-1)
[the energy of a wave increases with its frequency]
![Page 7: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/7.jpg)
AM Radio Waves
• KJR Seattle, Channel 95 (AM)950 kHz = 950,000 second-1
c = λν => λ = c/ν λ = 3.0x108 m s-1/ 9.5 x 105 s-1 = 316 m
When the frequency (ν) of EM is 950 kHz, the wavelength (λ) is 316 meters (about 1/5 mile).
![Page 8: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/8.jpg)
FM Radio Waves
• WABE Atlanta: FM 90.1 MHz c = λν => λ = c/ν
= 3.0x108 m s-1/ 90.1x106 s-1 = 3.33 m
FM radio waves are higher frequency, higher energy and longer wavelength, than AM radio waves.
![Page 9: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/9.jpg)
Problem
The X-ray generator in Loren Williams’ lab produces x-radiation with wavelength of 1.54 Å (0.1 nm = 1 Å). What is the frequency of the X-rays? What is the energy of each X-ray photon?
c = λν E = hν
![Page 10: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/10.jpg)
X-rays
X-rays were discovered in 1895 by German scientist Wilhelm Conrad Roentgen. He received a Nobel Prize in 1901. A week after his discovery, Roentgen took an x-ray image of his wife’s hand, visualizing the bones of her fingers and her wedding ring - the world’s first x-ray image.
Roentgen ‘temporarily’ used the term “x”-ray to indicate the unknown nature of this radiation. Max von Laue (Nobel Prize 1914) showed that x-rays are electromagnetic radiation, just like visible light, but with higher frequency (and higher energy) and smaller wavelength.
Within a few months of Roentgen’s discovery, doctors in New York used x-rays to image broken bones.
![Page 11: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/11.jpg)
c = λν E = hνProblem
The laser in an audio compact disc (CD) player produces light with a wavelength of 780 nm. What is the frequency of the light emitted from the laser?
![Page 12: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/12.jpg)
Problem
The brilliant red color seen in fireworks displays is due to 4.62 x 1014 s-1 strontium emission. Calculate the wavelength of the light emitted.
![Page 13: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/13.jpg)
Planck, Einstein, and Bohr
• 1901 Max Planck found that light (or energy) is quantized.
• In the microscopic world energy can be gained or lost only in integer multiples of hν.
ΔE = n(hν)n is an integer (1,2,3,…)
• h is Planck’s constant (h = 6.628X10-34 J s)
J: Joule, a unit of energy.
• Each energy unit of size hν is called a packet or quantum
![Page 14: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/14.jpg)
04/19/23 Zumdahl Chapter 12 14
• 1905 Einstein suggested that electromagnetic radiation can be viewed as a “stream of particles” called photons
Ephoton = hυ = h(c/λ)
• About the same time, Einstein derived his famous equation
E = mc2
• photons have mass.
![Page 15: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/15.jpg)
Dual nature of light
€
m =E
c 2
E = hν = hc
λ
⎛
⎝ ⎜
⎞
⎠ ⎟
![Page 16: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/16.jpg)
Electrons and Atoms: The Atomic Spectrum of Hydrogen (H.):
Put energy into a hydrogen atom (“excite it”),what comes out?
ie., at what energies does excited Hydrogen emit light?
![Page 17: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/17.jpg)
(1) A hydrogen atom consists of one electron and one proton.
(2) A hydrogen atom has discrete energy levels described by the primary quantum number n (1,2,3…) which gives the energy levels En (E1, E2, E3…)
(3) Light is emitted from a hydrogen atom when an electron changes from a higher energy state (Ebig) to a lower energy state (Esmall)
(4) The wavelengths emitted tell you ΔE2-1, ΔE3-1, ΔE2-4… (where ΔE2-1 = E2- E1).
(5) The observed emission spectrum of a hydrogen atom (at specific λ) tells you that the energy of a hydrogen atom is quantized.
n=1
n=2
n=4
€
E3 − E1
€
E2 − E1
€
E4 − E1n=3
![Page 18: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/18.jpg)
€
E3 − E2 = ΔE3−2 =hc
λ 656
€
E4 − E2 == ΔE4 −2 =hc
λ 486
€
E5 − E2 == ΔE5−2 =hc
λ 434
€
E2 − E1 == ΔE2−1 =hc
λ121
€
E3 − E1 == ΔE3−1 =hc
λ103
€
E4 − E1 == ΔE4 −1 =hc
λ 97
![Page 19: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/19.jpg)
The Bohr model of the hydrogen atom1. The hydrogen atom is a small, positively charged nucleus surrounded by a electron that travels in circular orbits. The atom is analogous to the solar system, but with electrostatic forces providing attraction, rather than gravity.
2. Unlike planets, electrons can occupy only certain orbits. Each orbit represents a discrete energy state. In the Bohr model, the energy of a hydrogen atom is quantized.
3. Light is emitted by a hydrogen atom when an electron falls from a higher energy orbit to a lower energy orbit.
4. Since each orbit is of a definite fixed energy, the transition of an electron from the higher energy orbit to the lower energy orbit causes the emission of energy of a specific amount or size (a quantum). The light emitted is at a specific frequency and wavelength.
![Page 20: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/20.jpg)
Electronic transitions in the Bohr model for the hydrogen atom
€
E3 − E1 = ΔE3−1 =hc
λ102
![Page 21: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/21.jpg)
Bohr calculated the angular momentum, radius and energy of the electrons traveling in descrete orbits.
€
En = −Z 2
n2 (2.18x10−18 J)
Calculated ΔE’s match observed λ(emission)
2
n 0
0
nr a radius of each orbital
Za called the bohr radius, a constant
n orbitals, excited states
n 1,2,3,... n 1 called ground state
Z is the postive charge on the nucleus
(1 of H, 2 for
= =
== =
He,etc.)
€
Angular Momentum = mevr
= nh
2π n = 1,2,3,.....
Bohr Model of the Atom (quantized energy)
![Page 22: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/22.jpg)
Modern Quantum Mechanics (1)
• Bohr recognized that his model violates principles of classical mechanics, which predict that electrons in orbit would fall towards and collide with the nucleus. Stable Bohr atoms are not possible.
• Modern quantum mechanics, with orbitals rather than orbits, provides the only reasonable explanation for the observed properties of the atoms
![Page 23: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/23.jpg)
Modern Quantum Mechanics (2)
• Orbital Defn: Orbitals are the “quantum” states that are available to electron. An orbital can be full (2 e-), half full (1e-), or empty. An orbital is a wave function, characterized by quantum numbers n (energy), l (shape), and m (direction).
• An orbital is used to calculate the probability of finding a electron at some location (Ψ2) – giving a three-dimensional probability graph of an electron position.
![Page 24: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/24.jpg)
Orbitals (like Standing Waves)
04/19/23 24
n=1 n=2 n=3
Analogy: An electron in an orbital can be imagined to be a standing wave around the nucleus. Electrons are not in the planet-like orbits.
![Page 25: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/25.jpg)
An orbital is a wavefunction (Ψ), described by three quantum numbers [ψ (n, l, ml)]
1. n = principal quantum numbern = 1, 2, 3, …n is related to the energy of the orbital
2. l = angular (azimuthal) quantum numberl = 0, 1, …. (n-1)l gives the shape of the orbitall = 0 is called an s orbital (these are spherical)l = 1 is called a p orbital (these are orthogonal rabbit ears)l = 2 is called a d orbital (these have strange shapes)l = 3 is called an f orbital (these have stranger shapes)l = 4 is called a g orbital (don’t even think about it)
ψ (n, l, ml)
ψ (n, l, ml)
![Page 26: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/26.jpg)
3. ml = magnetic quantum number
ml = -l, … , 0, ….+l
ml relates to the orientation of the orbital
Ψ (n, l, ml)
An orbital is a wavefunction (Ψ), described by three quantum numbers [ψ (n, l, ml)]
(continued)
![Page 27: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/27.jpg)
Quantum Numbers
Each orbital is specified by three quantum numbers (n, l, ml).
Each electron is specified by four quantum numbers (n, l, ml, ms).
ms = electron spin quantum number, indicated the electron’s spin, which can be up or down.
ms = +1/2, -1/2 denoted by ,
• Ψ (n, l , ml ) specifies an orbital.
• Ψ (n, l , ml , ms) specifies an electron in an orbital.
Ψ (n, l, ml)
![Page 28: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/28.jpg)
Electrons and Orbitals
• Each orbital is specified by 3 quantum numbers: (n,l,ml)
• Every orbital can hold two electrons
• Each electron is specified by 4 quantum numbers: (n,l,ml,ms)
![Page 29: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/29.jpg)
– n: the primary quantum number, controls size and energy, and the possibilities for l.
– l: the angular quantum number, controls orbital shape, and can also effect energy. l controls the possibilities for ml.
–ml: the orientation quantum number
Ψ (n, l, ml)
n l orbital designation
ml # of orbitals
1 0 1s 0 10 2s 0 11 2p -1, 0, +1 30 3s 0 11 3p -1, 0, +1 32 3d -2, -1, 0, +1, +2 50 4s 0 11 4p -1, 0, +1 32 4d -2, -1, 0, +1, +2 53 4f -3, -2, -1, 0, +1, +2, +3 7
2
4
3
Summary
![Page 30: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/30.jpg)
The First Three Orbitals Energy Levels (n=1,2 or 3)
Ψ (n, l, ml)
Ψ (1, 0, 0) Ψ(2, 0, 0)
Ψ (3, 0, 0)
Ψ(3, 1, -1)
Ψ (3, 1, 0)
Ψ(2, 1, -1)
Ψ(2, 1, 0)
Ψ(2, 1, +1)
n l orbital designation
ml # of orbitals
1 0 1s 0 10 2s 0 11 2p -1, 0, +1 30 3s 0 11 3p -1, 0, +1 32 3d -2, -1, 0, +1, +2 50 4s 0 11 4p -1, 0, +1 32 4d -2, -1, 0, +1, +2 53 4f -3, -2, -1, 0, +1, +2, +3 7
2
4
3
Ψ (3, 1, 1)
Ψ(3, 2,-2 )
Ψ (3, 2,-1 )
Ψ (3, 1, 0)
Ψ(3, 2, 1 )
Ψ (3, 1, 2)
![Page 31: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/31.jpg)
Ψ (n, 0, 0)
Ψ (1, 0, 0) Ψ (2, 0, 0) Ψ (3, 0, 0)
l = 0 s orbitals
Degeneracy
n2 = number of degenerate orbitals with the same energy (this applies to hydrogen only).
![Page 32: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/32.jpg)
Ψ (2, 1, ml)
Ψ (2, 1, -1)
Ψ (2, 1, 0)
Ψ (2, 1, +1)
l = 1 p orbitals
![Page 33: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/33.jpg)
Ψ (3, 2, -2) Ψ (3, 2, -1) Ψ (3, 2, 0)
Ψ (3, 2, 1) Ψ (3, 2, 2)
l = 2 d orbitals
Ψ (3, 2, ml)
![Page 34: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/34.jpg)
34
l = 3 f orbitals
Ψ (4, 3, -3) Ψ (4, 3, -2) Ψ (4, 3, -1)
Ψ (4, 3, 0) Ψ (4, 3, 1) Ψ (4, 3, 2) Ψ (4, 3, 3)
Ψ (4, 3, ml)
![Page 35: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/35.jpg)
From the graph:1. Are 2s and 2p degenerate (i.e., do they
have the same energy)?2. Which is lower energy? 4s or 3d?3. Which is lower energy? 6s or 4f?4. Which is lower energy? 3d or 4p?
Orbital Energy Levels of Atomswith many Electrons:
The degeneracy is lost.
![Page 36: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/36.jpg)
Energy Levels: Why is the 2s orbital higher in energy than a 2p orbital?
Penetration: Electrons in the 2s orbital are closer to the nucleus (on average) than electrons in a 2p orbital.
So 2s electrons shield the 2p electrons from the nucleus. This raises the energy of the 2p electrons (Coulomb’s law).
![Page 37: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/37.jpg)
Many Electron Atoms (2)Aufbau Principle
• The Aufbau principle assumes a process in which an atom is "built up" by progressively adding electrons and protons/neutrons. As electrons are added, they enter the lowest energy available orbital.
• Electrons fill orbitals of lowest available energy before filling higher states. 1s fills before 2s, which fills before 2p, which fills before 3s, which fills before 3p.
![Page 38: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/38.jpg)
Many Electron Atoms (3)Filling Orbitals with Electrons
1s (holds 2e-) then 2s (2e-) then2p (6e-) then3s (2e-) then3p (6e-) then4s (2e-) then3d (10e-) then4p (6e-) then5s (2e-) …
![Page 39: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/39.jpg)
Many Electron Atoms (4)
Pauli Exclusion PrincipleNo 2 electrons in an atom can have the same set
of quantum numbersn, l, ml, ms
ms = electron spin quantum numberms = +1/2, -1/2 denoted by
![Page 40: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/40.jpg)
– Every degenerate orbital is singly occupied (contains one electron) before any orbital is doubly occupied (Electrons distribute as much as possible within degenerate orbitals This is called the "bus seat rule” It is analogous to the behavior of passengers who occupy all double seats singly before occupying them doubly.
– Multiple electrons in singly occupied orbitals have the same spin.
Hund’s RulesMany Electron Atoms (5)
![Page 41: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/41.jpg)
Periodic Table
![Page 42: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/42.jpg)
The Quantum Mechanical Periodic Table
![Page 43: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/43.jpg)
Orbitals and the Periodic Table
![Page 44: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/44.jpg)
![Page 45: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/45.jpg)
The principle quantum number for the outermost 2 electrons in Sr would be:
1) 3
2) 4
3) 5
4) 6
5) none of the above
PRS Question
![Page 46: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/46.jpg)
The Angular quantum number (l) for the outermost electron on K is:
1) 0
2) 1
3) 2
4) 3
5) none of the above
PRS Question
![Page 47: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/47.jpg)
An electron in which subshell will on average be closer to the nucleus?
1) 3s
2) 3p
3) 3d
4) 4d
5) none, they are all the same
distance from the nucleus
PRS Question
![Page 48: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/48.jpg)
Which atom has a smaller 3s orbital?
1) An atom with more protons
2) An atom with fewer protons
3) An atom with more neutrons
4) An atom with fewer neutrons
5) The size of the 3s orbital is the
same for all atoms.
PRS Question
![Page 49: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/49.jpg)
– Every degenerate orbital is singly occupied (contains one electron) before any orbital is doubly occupied (Electrons distribute as much as possible within degenerate orbitals This is called the "bus seat rule” It is analogous to the behavior of passengers who occupy all double seats singly before occupying them doubly.
– Multiple electrons in singly occupied orbitals have the same spin.
Hund’s Rules
![Page 50: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/50.jpg)
04/19/23 Zumdahl Chapter 12 50
![Page 51: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/51.jpg)
1s 2s 2px 2py 2pz
1H:
2He:
3Li:
4Be:
5B:
1s1
1s2
1s22s1
1s22s2
1s22s22px1
“Aufbau” from Hydrogen to Boron
![Page 52: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/52.jpg)
1s 2s 2px 2py 2pz
6C:
7N:
8O:
9F:
10Ne:
1s22s22px12py
1
1s22s22px12py
12pz1
1s22s22px22py
12pz1
1s22s22px22py
22pz2
1s22s22px22py
22pz1
“Aufbau” from Carbon to Neon
![Page 53: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/53.jpg)
• Valence Electrons– can become directly involved in chemical bonding– occupy the outermost (highest energy) shell of an atom– are beyond the immediately preceding noble-gas configuration– among the s-block and p-block elements, include electrons in s and p
subshells only– among d-block and f-block elements, include electrons in s orbitals
plus electrons in unfilled d and f subshells
![Page 54: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/54.jpg)
Why is Silver Ion Ag+
• Why not Ag0 or Ag2+ or Ag3+? • What is the electron configuration for silver
(Ag0)?• What happens to the configuration if we
remove one electron from Ag0?
![Page 55: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/55.jpg)
Can you identify this element?
• 1s22s22p65p1
• Why is the electron configuration written as such? (why not 1s22s22p63s1)
• Is 1s22s22p6 a different element?
![Page 56: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/56.jpg)
What is the maximum number of electrons that can occupy the orbitals with principal quantum number = 4?
1) 2
2) 8
3) 18
4) 32
5) none of the above
PRS Question
![Page 57: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/57.jpg)
Which of the following have 4 valance electrons?
1) Al
2) Si
3) P
4) As
5) Be
PRS question
![Page 58: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/58.jpg)
What is the maximum number of electrons that can occupy the orbitals with principal quantum number = 3?
1) 2
2) 8
3) 18
4) 32
5) none of the above
PRS question
![Page 59: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/59.jpg)
Which of the following is the electron configuration of a ground state Se atom?
1) [Ar]4s24d104p4
2) [Ar]3s23d103p3
3) [Ar]4s23d104p3
4) [Ar]4s23d104p4
5) none of the above
PRS question
![Page 60: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/60.jpg)
What is the electron configuration of a phosphorous atom?
1) 1s22s23s22p63p2
2) 1s22s22p63s23p3
3) 1s22s22p63s23p2
4) 1s22s22p63p4
5) 1s22s22p63s4
PRS question
![Page 61: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/61.jpg)
How many unpaired electrons are on a phosphorous atom?
1) 2
2) 3
3) 4
4) 5
5) 6
PRS question
![Page 62: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/62.jpg)
How many valence electrons are there in a Cl atom?
1) 4
2) 5
3) 6
4) 7
5) 8
PRS question
![Page 63: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/63.jpg)
Problem:
Write the valance-electron configuration and state the number of valence electrons in each of the following atoms and ions: (a) Y, (b) Lu, (c) Mg2+
(a) Y (Yttrium): atomic number Z = 39
[Kr] 5s2 4d 1 3 valence electrons
(b) Lu (Lutetium): Z = 71
[Xe] 6s 2 4f 14 5d 1
(c) Mg2+ (Magnesium (II) ion): Z = 12
This is the 2+ ion, thus 10 electrons
[Ne] configuration or 1s2 2s2 2p6
0 valence electrons
3 valence electronsNote filled 4f sub shell
![Page 64: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/64.jpg)
Periodic Trends in Atomic Properties
• Ionization Energy
• Electron Affinity
• Atomic Radius
• Electronegativity
![Page 65: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/65.jpg)
Ionization energy of an atom is the minimum amount of energy necessary to detach an electron form an atom that is in its ground state.
X → X+ + e - ΔE = IE1 X+ → X2+ + e - ΔE = IE2
![Page 66: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/66.jpg)
The first ionization energy values decrease in going down a group
![Page 67: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/67.jpg)
X + e─ → X─ ΔE = electron attachment energy
EA tends to parallel IE, but shifted one atomic number lower
e.g. Halogens have a much higher EA than noble gases
Electron Affinity
![Page 68: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/68.jpg)
Electron Affinity
![Page 69: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/69.jpg)
Which of the following has the greatest magnitude?
1) The first ionization energy of strontium (Sr)
2) The first electron affinity of fluorine (F)
3) The second ionization energy of magnesium
(Mg)
4) The first ionization energy of oxygen (O)
5) The third ionization energy of magnesium
(Mg)
PRS
![Page 70: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/70.jpg)
Which of the following has the greatest magnitude?
1) The first ionization energy of strontium
2) The first electron affinity of fluorine
3) The second ionization energy of
magnesium
4) The first ionization energy of oxygen
5) The third ionization energy of
magnesium
PRS
![Page 71: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/71.jpg)
Electron Affinity vs Electronegativity
1. ELECTRON AFFINITY is the ENERGY RELEASED when an atom in the gas
phase adds an electron to form a negative ion: E + e(-1) ---> E(-1). This quantity can be measured experimentally.
Unfortunately, even though most electron affinities tend to be EXOTHERMIC,
They are given as positive quantities, which is the opposite the normal sign convention.
2. ELECTRONEGATIVITY is an empirical scale of the ability of an atom IN A COVALENTLY BONDED MOLECULE to attract electrons from other atoms in the molecule.
Electronegativity is related to but is no the same as electron affinity.
![Page 72: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/72.jpg)
Atomic Radius
The radius of an atom (r) is defined as half the distance between the nuclei in a molecule consisting of identical atoms.
![Page 73: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/73.jpg)
Atomic radii (in picometers) for selected atoms.
![Page 74: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/74.jpg)
Nuclear Charge
What does increasingthe nuclear charge do tothe orbital energy?
A. More PositiveB. Closer to ZeroC. More Negative
What does this mean?
![Page 75: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/75.jpg)
Shielding
![Page 76: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/76.jpg)
Sizes of Atoms and Ions
Atomic size generally increases moving down a group
Among s-block and p-block elements, atomic size generally decreases moving from left to right
![Page 77: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/77.jpg)
The Trend in Atomic Size
![Page 78: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/78.jpg)
Ions
Observations:
How does thistrend differfrom atoms?
Explain.
Think-Pair-Share
![Page 79: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/79.jpg)
PRS Question
What is the correct order of decreasing size of the
following ions?
A. P3- > Cl- > K+ > Ca2+
B. Ca2+ > K+ > Cl- > P3-
C. K+ > Cl- > Ca2+ > P3-
D. K+ > Cl- > P3- > Ca2+
![Page 80: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/80.jpg)
The “Trends”
![Page 81: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/81.jpg)
Iron Compounds
Fe
4s 3d 3d 3d 3d 3d 4p 4p 4p
4s 3d 3d 3d 3d 3d 4p 4p 4p
Fe3+
![Page 82: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/82.jpg)
PRS Question
47. Select the diamagnetic ion. A. Cu2+ B. Ni2+ C. Cr3+ D. Sc3+ E. Cr2+
![Page 83: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/83.jpg)
(1885-1962 )
Highlights– Worked with J.J. Thomson (1911) who
discovered the electron in 1896– 1913 developed a quantum model for
the hydrogen atom– During the Nazi occupation of Denmark
in World War II, escaped England and America
– Associated with the Atomic Energy Project.
– Open Letter to the United Nations in 1950 peaceful application of atomic physics
Moments in a Life– Nobel Prize in Physics 1922
Niels Bohr
![Page 84: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/84.jpg)
The Uncertainty Principle. In 1927, Werner Heisenberg established that it is impossible to know (or measure), with arbitrary precision, both the position and the momentum of an object
imprecision of position
imprecision of momentum
The better position is known, the less well known is momentum (and vice versa). π4
hvmx ≥Δ⋅Δ
Quantum Mechanics and Atomic Structure (Part 1)
![Page 85: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/85.jpg)
Heisenberg’s Uncertainty Principle:
You cannot measure/observe something without changing that which you are observing/measuring.
![Page 86: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/86.jpg)
Determine the position of an electron with the precision on the order of the size of an atom.
what is the uncertainty of the velocity, ∆v?
![Page 87: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/87.jpg)
Determine the velocity of an apple to be zero, but with uncertainty of 10-5 m/s
what is the uncertainty of the position, ∆x?
![Page 88: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/88.jpg)
The Heisenberg uncertainty principle:
1) places limits on the accuracy of
measuring both position and motion
2) is most important for microscopic
objects
3) makes the idea of “orbits” for
electrons meaningless
4) none of the above
5) a, b and c
PRS Quiz
![Page 89: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/89.jpg)
The Heisenberg uncertainty principle:
1) places limits on the accuracy of
measuring both position and motion
2) is most important for microscopic
objects
3) makes the idea of “orbits” for
electrons meaningless
4) none of the above
5) a, b and c
![Page 90: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/90.jpg)
For macroscopic objects, we can ignore the wave properties since m is large.
DeBroglie: Even baseballs are waves. Particles move with linear momentum (p) and have wave like properties and a wavelength
(λ = h/p = h/mev)
Quantum Mechanics and Atomic Structure (Part 2)
![Page 91: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/91.jpg)
Quantum Mechanics and Atomic Structure (Part 3)
Schrödinger EquationĤ = E
![Page 92: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/92.jpg)
Schrödinger EquationĤ = E
Results in many solutions, each solution consists of a wave function, (n, l, ml) that is a function of quantum numbers.
(x, y, z) is a complex function defined over three dimensional space. Its complex square is a three dimensional probability function, i.e 2 = the probability that an electron is in a certain region of space. 2 defines the shapes of orbitals.
The wave function provides a complete description of how electrons behave. Each n, l, ml describes one atomic orbital.
![Page 93: Chapter 12 Quantum Mechanics and Atomic Theory 5.1 Electromagnetic Radiation 5.2 The Nature of Matter 5.3 The Atomic Spectrum of Hydrogen 5.4 The Bohr](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649e225503460f94b0fd63/html5/thumbnails/93.jpg)
Schrodinger Eqn Solutions