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Title: Quantum Mechanics and Modern Physics


1
Quantum Mechanicsand Modern Physics
  • Science Engineering Magnet High
  • Mr. Puckett

2
First Atomic Theory
  • The notion that all matter consists of
    fundamental particles called atoms was first put
    forward by the Greek philosophers Leucippus and
    his disciple Democritus, in the 5th century BC.
  • These men taught that everything is composed of
    infinitely tiny indivisible particles called
    atoms. The word atom, from the Greek, means
    "indivisible."

3
First Atomic Theory continued
  • The notion of atoms was rejected by other
    philosophers--most significantly Aristotle, who
    believed all matter was infinitely divisible.
  • Others believed there were only four elements
    earth, air, fire, and water. These "nonatomic"
    beliefs dominated Western thought for centuries.
    Only in the early modern era did the concept of
    atoms regain acceptance. Today, however, atoms
    are known to be divisible into subatomic
    particles, such as electrons, protons, neutrons,
    and quarks1

4
John Daltons Atomic Theory
  • John Dalton's Atomic theory in the late 1700's
    explained the nature of chemical reactions and
    the similarity of certain elements. It
    included
  • A. All elements are composed of tiny indivisible
    particles called atoms. ( Incorrect in long run)
  • B. Atoms of the same element are identical.
  • C. Atoms of different elements can combine with
    one another to form compounds.
  • D. Chemical reactions occur when atoms are
    separated, joined or rearranged.

5
JJ Thompson discovers the Electron
  • The discoverer of the electron as a separate
    subatomic particle was J.J. Thompson in 1897.
    He realized that the accepted model of an
    indivisible atom did not take electrons and
    protons into account. He used a cathode ray tube
    that bent an electron beam in EM fields.
  • He suggested a revised model that was compared to
    a "plum pudding atom" because it said that
    negatively charged electrons (raisins) stuck into
    a lump of positively charged protons (the dough).

6
JJ Thompsons Cathode Ray Tube
  • Thompson generated electric rays by using a
    pair of oppositely charged plates that were set
    in an evacuated tube. When this was done, a
    small glowing spot appeared at the opposite end
    of the tube. Thompson noticed that if a magnetic
    field was applied to the beam, the spot on the
    opposite side of the tube moved. This implied
    that the ray was composed of a negatively
    charged particle which responded to the magnetic
    field according to the equation F qvB ma.

7
Thompsons Cathode Ray Tube
  • Thompsons CRT measured the charge to mass ratio
    and gave evidence of electrons.

8
Electrons from a CRT
  • What Thompson had discovered were electrons,
    which were being stripped off the cathode by the
    strong voltage as shown in the diagram. Although
    he was not able to see individual electrons, the
    amount of deflection they experienced while
    traveling through the tube depended upon the
    electrons mass and charge.

9
Millikans Oil Drop Experiment
  • Millikan used an atomizer to create tiny drops of
    oil that were given an electric charge and
    allowed to fall between two charged plates.
  • The mass of a given oil drop can be calculated by
    the rate at which it falls when the electric
    field is turned off. The electric field is then
    turned on and the drop is brought to a halt. At
    this point the electrical force on the drop and
    the gravitational force on the drop are equal
    (qEmg) and the total charge on each drop can be
    calculated.

10
Millikans Oil Drop Experiment
11
Determined the Elemental Charge on the Electron
  • After calculating the charge on many drops,
    Millikan noticed that the charge on each drop was
    always a multiple of a common factor, 1.6x10-19C,
    which he reasoned was the fundamental electric
    charge. Although he did not know it at the time,
    he had discovered the charge of the electron.

12
Ernest Rutherford Discovered the Nucleus with the
?- Gold Foil Lab
  • Ernest Rutherford discovered the nucleus in 1911
    and proposed the nuclear atom in which electrons
    surround a dense nucleus.
  • He thought of the rest of the atom as empty
    space. But the electrons are negatively charged
    and the nucleus (protons) are positively charged.

13
Rutherfords Discovery of the Nucleus with the
Gold Foil Lab
  • After the discovery that radioactive elements
    emitted rays of various types, physicists
    rushed out to shine beams of rays at different
    substances.
  • Rutherford shone a beam of alpha particles,
    actually a beam of helium nuclei, at a thin sheet
    of gold foil. Most alpha particles behaved as
    expected, being deflected slightly or not at all.
    However, occasionally an alpha particle would be
    knocked almost backwards.

14
The Dense Nucleus makes itself Known in a Big Way
  • Rutherford said, This unexpected result was
    equivalent to firing an artillery shell at a
    sheet of tissue paper and having the artillery
    shell bounce back!
  • These results implied that the alpha particles
    would occasionally strike a small, incredibly
    dense object Rutherford had discovered the
    nucleus!
  • Note this question was asked in both 82 and 97.

15
Rutherfords Gold Foil Lab
16
Rutherford Experiment CloseUp
17
The Bohr Atomic Model - (Solar System)
  • Neils Bohr developed the next stage of the atomic
    theory in 1913 with the Bohr model.
  • It proposes that the electrons are in concentric
    circular orbits around the nucleus. The model
    was patterned after our solar system with the sun
    in the center (nucleus) and the planets
    (electrons) orbiting around it.
  • The energy that the orbiting provides prevents
    the electrons from falling into the nucleus

18
Energy Levels of Electrons
  • The ENERGY LEVEL of an electron is the region
    around the nucleus where it is most likely to be
    found.
  • The different energy levels are analogous to the
    rungs of a ladder. The higher you go up the
    ladder (away from the nucleus) the higher the
    energy .
  • Electrons can also climb the ladder and jump
    from one energy level to the next ( energy must
    be provided or taken away in the proper amount).

19
Energy Orbitals of the Electrons
  • Electron energy orbitals are the regions where
    there is the greatest chance to find them as
    clouds

20
Electron Orbitals
  • Electrons cannot stay between levels and will
    naturally migrate to their appropriate level.
    However, unlike the rungs of a ladder, the energy
    levels are not equally spaced.
  • A QUANTUM of energy is the amount of energy
    required to move an electron from its present
    energy to the next higher level. Thus the
    energies of electrons are said to be quantized.
    The term , quantum leap, is used to describe an
    abrupt change

21
The Birth of Quantum Mechanics
  • It all began when Max Planck (1900) was trying
    to explain the glow of a hot glowing blackbody
    like an electric stove eye.
  • A black object absorbs all wavelengths of light,
    yet glows red with high temperature. Higher temps
    yield yellow and white light. The spectrum fit an
    empirical formula when he assumed that the energy
    was not continuous, but small discrete amounts.
    These amounts were called Quanta

22
Origin of the Word Quantum
  • The light emitted by a glowing piece of iron, for
    instance, was actually "grainy," composed of
    minuscule light "grains" too small to be seen.
  • Planck called a light "grain" a quantum, from the
    Latin word meaning "how much?"

23
Temperature and Wavelength of Light
  • Weins Law was the basis for the wavelength
    calculations based upon temperature for Plancks
    energy constant.
  • Formula ? T 2.9 x 10-3 m.K

24
Quanta comes in Specific Amounts
  • Planck proposed that electrons, for some unknown
    reason, can give off light only in certain
    specific amounts of light energy--in quanta.
  • Only whole quanta can be given off, never a
    fraction of a quantum.
  • The energy of these quanta varies directly with
    the frequency of the light. Energetic light of
    higher frequency, such as violet or ultraviolet
    light, consists of higher-energy quanta than does
    light of lower frequency, such as red or infrared
    light.

25
Plancks Constant Describes the Energy of a
Quantum
  • The energy of Plancks constant is the energy
    needed to promote electrons to the next higher
    energy orbital based upon frequency. E hf
  • The formula became Enhf where n is the
    whole number multiple of h (Plancks constant
    6.6 x10-34 J.s) and f is the frequency of
    light photons.

26
Plancks Constant of KE vs. Frequency
27
Plancks Constant Energy Level
  • Planck's constant is expressed in terms of energy
    multiplied by time--a unit called action--and may
    be given in erg-seconds or joule-seconds. An erg
    is defined as the amount of energy needed to
    raise a milligram (roughly the weight of a grain
    of sand) a distance of 1 centimeter (about 1/3
    inch). This is not a great deal of energy.

28
Einstein Uses Plancks Constant for the
Photoelectric Effect
  • In 1905 the German-born physicist Albert Einstein
    used Planck's quantum theory to explain the
    photoelectric effect, in which charged particles
    such as electrons are emitted from certain
    materials when light (electromagnetic radiation)
    strikes the materials - mostly metals.
  • This is the topic of Einsteins Nobel Prize- not
    Relativity.

29
Plancks Threshold Electron Ejection
30
Einstein Explained Plancks Constant with the PE
of the Photoelectric Effect
  • Albert Einstein said that the electrons around an
    atom were trapped in a potential energy well.
    If an electron was to escape the well it would
    have to be struck by a single photon of light
    which would have enough energy to kick the
    electron out of the well.  
  • Chemists call this the ionization constant the
    amount of energy needed to remove electrons.
  • This question was asked on the AP test in 1997.

31
The KE of Electrons with Escape Velocity from the
Atom
  • Photons with a frequency of fo have just
    enough energy to accomplish this. Photons with
    higher frequencies not only have enough energy
    for the electron to escape, but have extra energy
    to give the electron additional kinetic energy,
    KEmax in the diagram.

32
Work Function Exciting the Electrons Up
  • The Energy required to take the electron from the
    one level and promote it to a higher level is
    found with the Work Function W?E hfo
    where h is Plancks constant and fo is the
    threshold frequency to promote the electron.
  • The KE of an ejected electron is the quantum
    energy the work function. KE hf hfo .
    The difference is the amount of energy for the
    kinetic energy ½ mv2.

33
Photon Energy Problem
34
Photon Speed and Energy
35
Photoelectric Effect Diagram
  • In this lab the light shines on the metal and has
    enough energy that it knocks electrons off the
    metal into a detector that causes a current
    through the circuit.

36
Einstein proposes Quanta Energy Levels of
Electrons
  • Einstein also proposed that electrons, besides
    emitting electromagnetic radiation in quanta,
    also absorb it in quanta.
  • Einstein's work demonstrated that electromagnetic
    radiation has the characteristics of both a
    wave--because the fields of which it is composed
    rise and fall in strength--and a
    particle--because the energy is contained in
    separate "packets." These packets were later
    called PHOTONS.

37
Comptons Scattering Effect
  • This experiment was similar to the Rutherfords
    experiment except that the beam was composed of
    particles of light, called photons. In this case
    a photon stuck an atom, knocked an electron off
    the target, and was then deflected. The only way
    a photon can knock an atom out of an electron
    is if the photon had momentum. This suggested
    that photons were particles.
  • However, the scattered photon did not seem to
    change speed during the collision, but rather
    changed their frequency.

38
Comptons Scattering Effect
  • This suggested that photons were actually waves
    that travel at the speed of light, changing
    frequency as energy is lost.
  • Comptons conclusion? Photons can act as both
    waves and as particles depending on the
    situation. This question was asked in 1982.

39
Michelson Morley Determined the Speed of Light
  • Michelson and Morley first proposed the
    experiment to find the speed of the Earth through
    the ether that filled the universe.
  • A single beam of light was split into two paths
    and then rejoined at an observation scope. If
    the Earth was traveling to the right through the
    Ether Wind the light traveling at right angles
    to the wind would be blown off course and
    require more time to reach the telescope.

40
Michelson Morley Experiment Continued
  • By allowing the two beams to interfere with each
    other, sight differences in the speed of the two
    beams could be calculated. By measuring the
    difference in the speed of the two beams, the
    speed of the Earth through the Ether could be
    worked out.
  • It turned out that no matter how the experiment
    was set up, the speed of light in both directions
    remained constant. Thus no Ether.
  •  Note Although this question was asked in both
    1982 and 1987, relativity is no longer on the AP

41
Michelson-Morley Experiment
  • The Michelson- Morley Interferometer was used to
    measure the speed of light and measure the
    Ether. It never found the ether, but did
    establish 2.99 x 10 8 m/s as the speed of light.

42
Nuclear Reactions
  • It was originally thought that the fundamental
    particle of matter was the atom and that atoms
    could neither be created nor destroyed.
  • The discovery that atoms were made up of protons,
    neutrons, and electrons suggested the possibility
    that one type of atom could be transformed into
    another type of atom by adding or subtracting
    these fundamental particles.
  • The reactions are either FUSION or FISSION.

43
Nuclear Fusion in the SUN !
  • This happens every day as hydrogen isotopes are
    transformed into helium in the sun.
  • In this type of equation, atoms are written in
    the form where X is the atomic symbol, Z is the
    atomic number of the atom (basically the number
    of protons an atom contains) and A is the mass
    number of the atom (the total number of protons
    and neutrons in the atom). AZX Example 21H is
    deuterium (heavy hydrogen)

44
Nuclear Fusion Formula
  • Fusion is the nuclear reaction that combines the
    hydrogen isotopes into helium and releases huge
    amounts of energy as in the sun and stars.
  • The equation is 21H 31H ? 42 He 10n E

45
Nuclear Fission Reaction
  • Fission is the process of breaking down the
    nucleus by physical bombardment with neutrons of
    other decaying radioactive atoms.
  • This is the type of reaction that is used in
    modern nuclear reactors and was the first Atomic
    Bomb mechanism.

46
Nuclear Fission Reaction
  • As the first nucleus decays it gives off 3
    neutrons that strike other atoms and cause them
    to decay in a cascading reaction.

47
Nuclear Power Reactor
  • A nuclear reactor is a complex heat exchanger
    with a steam driven generator.

48
The Infamous E mc2
  • Under normal conditions, the total number of
    fundamental particles in an atomic reaction
    remains constant. The exception usually occurs
    in particle accelerators, black holes, and other
    unpleasant environments where there is enough
    excess energy to create new matter according to
    the Einsteins equation Emc2.
  • An electron and a proton can also combine to form
    a neutron, which usually occurs only under very
    high pressures.

49
Mass and Energy are Equivalent
  • Atoms form because it requires less energy for
    two protons and two neutrons to exist as a He
    atom than as separate particles.
  • Since Einstein showed that mass and energy are
    equivalent (Emc2) we can directly measure the
    energy content of atoms by measuring their mass.

50
The Loss of Mass in Fusion gives ENERGY !!
  • Since He consists of two protons and two
    neutrons, we can estimate the mass of a He atom
    as 2(mn1.008665 au) 2(mp1.007825 au)
    4.032980 au
  • However, the measured mass of the He atom is
    only 4.002603 au, a difference of 0.0030377 au.

51
Energy Release from Fusion
  • This mass deficit may seem small, but if we use
    Einsteins formula to convert this mass into
    energy we get Emc2
  • E (0.00303)(6.66x10-27 kg)(3x108m/s)2
    4.5 x10-13 Joules.
  • This does not seem like a lot of energy, but
    remember this is for just one atom. The process
    of making a mole of He atoms releases 2.7x1011 J

52
Radioactive Decay The Three Products
  • The weak nuclear force in nature is responsible
    for Radioactive Decay the spontaneous splitting
    of radioactive isotopes gradually into more
    stable elements and energy release.
  • There are three decay products the Alpha
    particle, Beta particle and the Gamma Ray.

53
Decay Particles from Fission
  • The Alpha particle (??) is the nucleus of the
    Helium atom. When it is given off the atomic
    number reduces by 2 and mass number by 4 and
    changes to a new element.
  • The Beta particle (?) is a high speed electron
    from a neutron and leaving a proton that
    increases the atomic number by 1.
  • The Gamma Ray (?) is an energy ray without mass.

54
Alpha Particle Decay
  • Example When Uranium-238 decays by an alpha
    decay the result is a helium nucleus and a
    thorium-234 atom. Notice that as in any
    chemical equation, the summation of the mass
    before and after the reaction adds up.
  • 23892 U ? 42He 23490Th

55
Beta Particle Emission
  • The beta particle is actually a high speed
    electron. It originates from the decay of a
    neutron (0) in the nucleus into a proton(1) and
    an electron(-1). This causes a change of 1 to
    the atomic number and a ZERO change to the Mass
    number. Remember the electron is 1/1830 the mass
    of a proton.
  • Example If an carbon-14 decays into a
    nitrogen-14 the formula looks like
  • 146C ? 147N e- a neutrino

56
Gamma Emission
  • The gamma emission is a photon of very high
    energy. The decay of a nucleus by emissions of a
    gamma ? ray is much like emission of photons by
    excited atoms. Except this time it is an excited
    nucleus with a lot more energy. Since it is only
    energy, there is NO CHANGE in mass or charge.
    Gammas are deadly ionizing radiation. Neutron
    bombs work from this mechanism.
  • AZ N ? AZ N ?

57
Radioactive Half Life
  • The half-life of a radioactive material is the
    amount of time it takes for ½ of the mass of a
    radioactive isotope sample to decay spontaneously
    into new material. Two versions of the formula
    are ?N - ?N ?t and N Noe-?t where ? is
    the decay constant and N is the number of
    radioactive nuclei. The shortcut formula is T ½
    0.693/ ?
  • Half-lives can range from a fraction of a second
    to billions of years. Carbon-14 has a ½ life of
    5370 years while U-238 has a 2.3 billion year
    half life.

58
Erwin Schrodingers Wave Equations for Electron
Orbitals
  • Erwin Schrodinger took the atomic model another
    step in 1926, when he used the new quantum theory
    to write and solve an equation describing the
    location and energy level of an electron.
  • The most modern description of the position of
    the electrons is the Quantum Mechanical Model.
    It is not a description of an exact pathway of
    the electron but is concerned with the likelihood
    of finding an electron in a certain position.
    The mathematical probability is artistically
    portrayed as a blurry cloud of negative charge.

59
The Quantum Atom Model
  • QUANTUM MECHANICAL MODEL of the atom designates
    the energy levels of electron and are designated
    by 4 numbers to describe the energy level,
    orbital and sub-orbital and the spin property.

60
Quantum Mechanics of Atomic Orbitals
  • ATOMIC ORBITALS are regions in space where there
    is a high probability of finding an electron.
    There are a maximum of two electrons per orbital.
    They will fill the atomic orbitals in a specific
    filling pattern.
  • Quantum Mechanics is an accounting system to map
    out the electrons of an atom.

61
Quantum Numbers of Hydrogen
  • The Principle Quantum number is an integer value
    of the energy orbital.
  • The Orbital quantum number is the orbital type
    s, p, d, f
  • The Magnetic quantum number is the direction of
    the angular momentum.
  • The Spin quantum number is the direction of
    electron rotation ½ or - ½ that gives rise
    to the magnetic properties within the structural
    domain.

62
Quantum Numbers for Electrons
63
Atomic Orbital Shapes
  • Different atomic orbitals are denoted by letters.
  • S - orbitals are spherical clouds.
  • P-orbitals give pear or dumbbell-shaped clouds.
    The shapes of d-orbitals and f-orbitals are more
    complex than what we will study this year.
  • Just as the clouds in the sky that you see,
    these clouds of probability are not sharp edged.
    They just gradually disappear.

64
Light and Atomic Spectra
  • The work that led to the development of the
    quantum mechanical model came from the study of
    light.
  • Light is considered to consist of
    electromagnetic waves that travel in a vacuum at
    the speed of 3 x 108 meters per second.
  • Spectroscopy is the study of the light emitted by
    the electrons when they undergo quantum leaps.

65
Wave Nature of Matter
  • The properties of light had been debated and
    researched for years. The photoelectric effect,
    Compton effect and others predict particle
    nature. Youngs double slit and Comptons
    experiments showed the wave nature.
  • In 1923 Louis de Broglie proposed that all matter
    (not just photons) had wave properties.

66
De Broglie Wavelength of Matter
  • De Broglie proposed that the wavelength of a
    material particle would related to its momentum
    with the equation
  • ? h/mv

67
  • deBroglie wavelength problem

68
Heisenberg Uncertainty Principle
  • In 1927 Walter Heisenberg developed the
    uncertainty principle that explains why we cannot
    measure the position and momentum of an object
    (electrons) precisely at the same time.
  • We can measure either property accurately, but
    not both due to the nature of matter / wave
    duality.
  • Another form of the same idea relates energy and
    time. If we measure the position of a photon,
    then ?x ? ? and ?t ?x/c so ?t ?/c

69
Heisenberg Uncertainty Example
  • An analogy of the uncertainty in measurement
    concept is this picture that you cannot measure
    the location of cars due to speed.

70
Heisenberg Uncertainty Principle
71
Heisenberg Uncertainty Problem
72
Position Uncertainty of Electron
73
Wavelength of an Electron
74
Photoelectron Speed and Energy
75
Atomic Spectroscopy
  • Atomic Spectroscopy is the analytical measurement
    of the quantum energy level jumps of different
    electron energy states.
  • It is a spectral analysis of the colors that an
    atom gives off (or takes in) when it changes
    energy levels.
  • It involves either Emission spectroscopy or
    Absorption spectroscopy.

76
Atomic Emission Spectroscopy
  • In this technique, the atoms are heated up to the
    point that the thermal energy promotes the
    electron up to an excited energy level and then
    measures the color (wavelength) of light that is
    given off when the electron collapses back into
    the ground state.

77
Energy Level Transitions of Electrons
78
Spectrum Examples
79
Energy of Photon Example Problem
80
Wavelength Problem in Spectroscopy
81
Lasers
  • A laser is a device that can produce a very
    narrow intense beam of monochromatic coherent
    light.
  • Coherent means that across any cross section of
    the beam, all parts would have the same phase.
  • It uses stimulated emission to stay in phase An
    excited electron is stuck by a photon of the
    same energy gives off a double photon.

82
Laser Stimulated Emission
  • When a photon of light at the same frequency hits
    an excited electron The electron produces
    coherent E M

83
AP Problems on Quantum Mechanics and Modern
Physics
  • Historical Physics Atomic Physics
  • 1982 7 1996 5
  • 1997 6 1999 4
  • Atomic Energy Levels Photoelectric Effect
  • 1992 4 1980 3
  • 1995 4 1988 6
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