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Atomic Physics

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Title: Atomic Physics


1
Atomic Physics
  • Chapter 28

2
Atomic Models
3
Introduction
  • How do neon signs work?

4
  • Our main focus will be on the hydrogen atom.
  • It is the simplestatomic system.

5
  • Why is it important to study the hydrogen atom?
  • Studying the quantum numbers for the allowed
    states of hydrogen will help us to describe the
    allowed states of more complex atoms.
  • The hydrogen atom is an ideal system for relating
    theory to experimentation.
  • Much that we learn about hydrogen can be extended
    to single electron ions like He and Li.

6
Early Models Of The Atom
  • The Greek model
  • Tiny, hard, indestructible sphere
  • 3

7
  • The J. J. Thomson model
  • A volume of positive charge is embedded with
    negative charges called electrons

8
  • The Rutherford model
  • A positive nucleus orbited by electrons.
  • The nucleus contains 99.9 of the atoms mass

9
  • The Rutherford model
  • Which force holds the electrons in orbit?
  • The Coulomb force

10
Problems with the Rutherford Model
  • There were two basic difficulties with the
    Rutherford model.
  • It could not explain why atoms radiate discrete
    frequencies.
  • Accelerating electrons should radiate
    electromagnetic waves.

11
Electron Transitions
  • Using a high voltage to move electrons through a
    gas causes the gas electrons to become excited
    and to jump from lower energy levels to higher
    energy levels.
  • Photons of various wavelengths are produced when
    electrons fall from higher energy levels to lower
    energy levels.

12
Emission Spectra
  • The emission spectrum of hydrogen
  • Can be produced by applying a high voltage across
    an evacuated glass tube filled with hydrogen
  • The observed wavelengths are characteristic only
    of hydrogen
  • 279, 57

13
The Balmer Series
  • In the Balmer Series
  • nf 2
  • There are four prominent wavelengths
  • 656.3 nm (red)
  • 486.1 nm (green)
  • 434.1 nm (purple)
  • 410.2 nm (deep violet)
  • 278, 28.7

14
Balmer Wavelengths
15
The Balmer Series Wavelength Equation
  • RH is the Rydberg constant
  • RH 1.0973732 x 107 m-1

16
Two Other Important Series
  • Lyman series (UV)
  • nf 1
  • Paschen series (IR)
  • nf 3
  • 70

17
Spectral Lines
  • How many different spectral lines could be
    produced by an electron in the n 3 state?
  • Three

18
  • How many different spectral lines could be
    produced by an electron in the n 4 state?
  • Six

19
Photon Energy
  • The equation for determining the energy of the
    emitted photon in any series

20
The Absorption Spectrum
  • An element can absorb the same wavelengths that
    it emits.
  • The spectrum consists of a series of dark lines.

21
Identifying Elements
  • The absorption spectrum was used to identify
    elements in the solar atmosphere were identified
    in this way.
  • Helium was discovered.

22
Thermal vs. Atomic Spectra
  • How could you tell if the light from a candle
    flame is thermal or atomic in origin?

23
  • If the spectrum is continuous, the source must be
    thermal.

24
Auroras
  • What is the origin of the colors in the aurora
    borealis?

25
  • High speed particles from space interact with the
    earths magnetic field.

26
The Bohr Theory Of Hydrogen
  • At the beginning of the 20th century, scientists
    wondered why atoms only radiated certain
    wavelengths.
  • Bohr provided an explanation.

27
Four Assumptions of The Bohr Theory
  • 1) The electron orbits the proton due to the
  • Coulomb force which produces centripetal
  • acceleration.

28
  • 2) Only certain electron orbits are stable
  • and do not radiate energy.

29
  • 3) Radiation is only emitted when an
  • electron drops from a more energetic
  • state to a lower state.

30
  • 4) The radius of the electrons orbit is
  • determined by the electrons orbital
  • angular momentum.
  • 28.6

31
Total Energy of the Hydrogen Atom
  • The total energy of the hydrogen atom can be
    determined by using this equation.

32
The Bohr Radius
  • An electron can exist only in certain allowed
    orbits determined by the integer n.
  • When n 1, we have what is known as the Bohr
    radius (ao).
  • ao 0.0529 nm

33
Orbital Radii
  • A general equation for finding the radius of any
    orbit

34
Energy States
  • The energy for various energy states can be found
    by using
  • n 1 is the ground state

35
Ionization Energy
  • The minimum energy required to ionize the atom is
    called the ionization energy.
  • An electron is completely removed from the atom.

36
The Hydrogen Spectrum
  • The general expression for determining
    wavelengths of the various series in the hydrogen
    spectrum

37
Bohrs Correspondence Principle
  • Quantum mechanics is in agreement with classical
    physics when the energy differences between
    quantized levels are very small.

38
Successes of the Bohr Theory
  • It accounted for the Balmer series and other
    series.

39
  • It predicted a value for the Rydberg constant
    that agreed strongly with the experimental value.

40
  • It gave an expression for the radius of the
    hydrogen atom.

41
  • It predicted the energy levels of hydrogen.

42
  • It also works with hydrogen-like (one electron)
    atoms.
  • Singly ionized helium

43
  • It also works with hydrogen-like (one electron)
    atoms.
  • Doubly ionized lithium

44
  • It also works with hydrogen-like (one electron)
    atoms.
  • Triply ionized beryllium

45
Four Quantum Numbers
  • The state of an electron is specified by four
    quantum numbers.
  • These numbers describe all possible electron
    states.
  • The total number of electrons in a particular
    energy level is given by

46
Principle Quantum Number
  • The principal quantum number (n) where n 1, 2,
    3,
  • Determines the energy of the allowed states of
    hydrogen
  • States with the same principal quantum number are
    said to form a shell
  • K, L, M, (n 1, 2, 3, )

47
Orbital Quantum Number
  • The orbital quantum number (l) where l ranges
    from 0 to (n 1) in integral steps
  • Allows multiple orbits within the same energy
    level
  • Determines the shape of the orbits
  • States with given values of n and l are called
    subshells
  • s (l 0), p (l 1), d (l 2), f (l 3), etc

48
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49
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50
Electron Subshells
51
  • Generally, the electrons in the s subshell are at
    the lowest energy level and those in the f
    subshell in the highest shell occupy the highest
    energy level.

52
  • As the shell number (n) increases the energy
    difference between the shells diminishes, as
    shown by the decreasing distance between each
    successive shell.

53
Electron Subshells
54
Magnetic Quantum Number
  • The magnetic quantum number (ml) where ml ranges
    from - l to l in integral steps
  • Explains why strong magnetic fields can cause
    single spectral lines to split into several
    closely spaced lines
  • Called the Zeeman effect

55
Spin Magnetic Quantum Number
  • The spin magnetic quantum number (ms) where ms
    can only be 0.5 or 0.5
  • Accounts for the fine structure of single
    spectral lines in the absence of a magnetic field

56
Hydrogen Like Atoms
  • Two important equations for hydrogen-like atoms
  • Orbital energy
  • Orbital radius

57
Angular Momentum
  • Physicists agreed that angular momentum was
    quantized but no one was able to explain why.
  • 28.10

58
Electron Standing Waves
  • de Broglie stated that an electron orbit would be
    stable if it contained an integral number of
    electron wavelengths.
  • Analogous to standing waves in a string

59
Wave Properties
  • It became generally agreed upon that wave
    properties were involved in the behavior of
    atomic systems.

60
Quantum Mechanics And The Hydrogen Atom
  • A review of the various quantum number ranges
    which are used to determine allowable states
  • n can range from 1 to infinity in integral steps
  • l can range from 0 to (n - 1) in integral steps
  • ml can range from l to l in integral steps
  • ms can only be ½ or ½

61
The Spin Magnetic Quantum Number
  • The spin magnetic quantum number explains the
    splitting of each energy level into two (the
    Zeeman Effect).
  • It explains how two very closely spaced lines may
    be formed in the spectra of certain gases.
  • Electron spin (spin-up and spin-down)

62
Questions
  • 2, 8, 12
  • Pg. 910

63
Electron Clouds
  • The electron may be found at various distances
    from the nucleus but the probability of finding
    it at a distance corresponding to the first Bohr
    orbit is a maximum.
  • It can be found in a spherical region known as
    the electron cloud.
  • 281, 282

64
The State of an Electron
  • The state of an electron is specified by four
    quantum numbers.
  • These numbers describe all possible electron
    states.
  • The total number of electrons in a particular
    energy level is given by

65
The Pauli Exclusion Principle
  • Two electrons in an atom can never have the same
    set of quantum numbers.
  • Because of this, the elements all have different
    chemical properties.
  • The n 1 energy level is filled with electrons
    first.

66
The Pauli Exclusion Principle And The Periodic
Table
  • Mendeleev arranged the elements in a periodic
    table according to their atomic masses and
    chemical similarities.
  • He left gaps which were filled in within the next
    20 years.
  • Vertical columns have similar chemical
    properties.
  • 15

67
The Periodic Table
68
Special Groups Within the Periodic Table
  • Noble gases
  • The outer shell is filled.
  • Alkali metals
  • The outer shell has only one electron.
  • Halogens
  • The outer shell needs one electron.

69
The Dow Corning Periodic Table
70
X-Rays
  • X-rays are emitted when a metal target is
    bombarded with high-energy electrons to produce
  • A broad continuous band
  • Bremsstrahlung
  • Characteristic x-rays
  • K??and K?
  • 284, 285

71
X-Ray Photons
  • What can the incoming electron from an electron
    gun do to a K-shell electron in a tungsten target
    atom?
  • It can knock a K-shell electron out of its energy
    level. Then, an electron from a higher energy
    level can fall into the K-shell (n 1).
  • The energy lost by the falling electron shows up
    as an emitted x-ray photon.

72
Characteristic X-Rays
  • K-shell emission produces higher-intensity x-rays
    than Bremsstrahlung.
  • The x-ray photon comes out at a single
    (characteristic) wavelength.
  • K??or K?

73
Ka X-Rays
  • When an incoming electron forces an electron out
    of the K shell an electron can drop down from the
    n 2 level and a Ka x-ray photon is emitted.

74
Kb X-Rays
  • When an incoming electron forces an electron out
    of the K shell an electron can drop down from the
    n 3 level and aKb x-ray photon is emitted.

75
  • Which x-ray photon has the highest energy?

76
Ka X-Ray Wavelengths
  • The wavelength of the emitted Ka x-ray
    photon is given by

77
Electron Shielding
  • One electron in the K shell partially shields the
    other from the charge of the nucleus.
  • Because of this, we use Zeff (Z - 1) in the Ka
    equation.

78
K? X-Ray Wavelengths
  • The wavelength of the emitted K? x-ray
    photon is given by

79
Electron Shielding
  • One electron in the K shell and eight electrons
    in the L shell partially shield the M-shell
    electrons from the charge of the nucleus.
  • Because of this, we use Zeff (Z - 9) in the K?
    equation.

80
Atomic Transitions
  • Atoms will only emit or absorb EM radiation at
    certain frequencies corresponding to transitions
    involving the various energy states.

81
Stimulated Absorption
  • In the stimulated absorption process, light may
    be used to stimulate electrons to higher excited
    states.
  • Only certain frequencies will do this.
  • 28.17

82
Spontaneous Emission
  • When the electrons randomly fall back to their
    original orbits we call this spontaneous
    emission.
  • 286

83
Spontaneous Emission
84
Stimulated Emission
  • In stimulated emission, all of the electrons can
    be made to fall back at the same time and thus
    produce bright, coherent light.
  • This is the basis for the operation of LASERS.

85
Stimulated Emission
86
Lasers
  • LASER - Light Amplification by Stimulated
    Emission of Radiation

87
Population Inversion
  • In a laser, electrons are stimulated so that
    there are more electrons in the excited state
    than in the ground state.
  • This is called a population inversion.
  • 287

88
Laser Requirements
  • There are three conditions for laser action to
    occur.
  • A population inversion
  • The excited state must be a metastable (long
    lifetime) state.
  • The photons must be confined long enough to
    stimulate further emissions.

89
He-Ne Lasers
  • The operation of a He-Ne laser
  • An oscillator is used to sweep electrons through
    a thin glass tube containing a He-Ne mixture.
  • The neon atoms are raised to a metastable state
    by collisions with excited helium atoms.
  • Electrons simultaneously returning to a lower
    energy state emit coherent photons of a
    particular wavelength. (632.8 nm)
  • 28.22a, 71, 288

90
Laser Frequencies
  • Frequency ranges of lasers
  • Infrared (CO2)
  • Visible (red, green, blue)
  • Ultraviolet

91
Laser Applications
  • Medical
  • Welding detached retinas
  • Laser surgery
  • Laser vision correction (Lasik)

92
Lasik Surgery
  • An ultra-thin flap is created on the eye's
    surface during LASIK corrective eye surgery.
    After laser energy is applied to reshape the eye,
    the flap is replaced to serve as a type of
    natural bandage.

93
  • Surveying and distance measurement

94
  • Cutting and drilling metals in industry

95
  • Fiber optic communications

96
Holography
  • Used in the production of three-dimensional
    images
  • Interference patterns are placed on film.
  • Used to protect credit cards
  • 283, 284

97
Making Holograms
98
CDs and DVDs
  • Information is stored in binary form.
  • Pits and land areas (ones and zeros)
  • The laser beam follows a spiral path.
  • A diffraction grating is used to provide
    tracking.
  • 40 second memory for music CDs

99
Infrared Remote Control
  • A different infrared wavelength is assigned to
    each number or function.
  • TV and stereo remote controls use IR.
  • Some computers and calculators use IR.
  • My MAC PowerPoint remote uses RF.
  • Dont confuse IR with RF controls.
  • MAC Photo Booth Demo

100
Semiconductor Devices
  • Doping
  • Donor atoms
  • N-type semiconductor
  • Acceptor atoms
  • P-type semiconductors

101
Semiconductor Devices
  • P-N junctions
  • Diodes
  • Forward bias
  • Reverse bias
  • Half-wave rectifiers
  • Full-wave rectifiers
  • Transistors

102
Transistors
  • Junction transistors
  • Types
  • npn
  • pnp
  • Parts of a transistor
  • Emitter
  • Base
  • Collector
  • 227

103
Semiconductor Devices
  • Integrated circuits
  • What are they?
  • Where are they used?
  • What are the advantages of integrated circuits?

104
Computer Memory
105
Questions
  • 7, 9 - 11, 15
  • Pg. 910
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