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    Chapter 2: Quantum Mechanics and Atomic Theory

    Chapter 12: Phenomena

    Phenomena: Different wavelengths of electromagnetic radiation were directedonto two different metal sample (see picture). Scientist then record if anyparticles were ejected and if so what type of particle as well as the speed of theparticle. What patterns do you see in the results that were collected?

    KExp.

    Wavelength of LightDirected atSample

    IntensityWhere Particles

    EjectedEjectedParticle

    Speed ofEjected Particle

    1 5.410-7 m Medium Yes e- 4.9104

    2 3.310-8 m High Yes e- 3.5106

    3 2.0 m High No N/A N/A

    4 3.310-8 m Low Yes e- 3.5106

    5 2.0 m Medium No N/A N/A

    6 6.110-12 m High Yes e- 2.7108

    7 5.5104 m High No N/A N/A

    FeExp.

    Wavelength of LightDirected atSample

    Where ParticlesEjected

    EjectedParticle

    Speed ofEjected Particle

    1 5.410-7 m Medium No N/A N/A

    2 3.410-11 m High Yes e- 1.1108

    3 3.9103 m Medium No N/A N/A

    4 2.410-8 m High Yes e- 4.1106

    5 3.9103 m Low No N/A N/A

    6 2.610-7 m Low Yes e- 1.1105

    7 3.410-11 m Low Yes e- 1.1108

    EjectedParticle

    ElectromagneticRadiation

    Chapter 12:QuantumMechanics andAtomic Theory

    o Electromagnetic

    Radiation

    o Quantum Theory

    o Particle in a Box

    o The Hydrogen Atom

    o Quantum Numbers

    o Orbitals

    o Many Electron Atoms

    o Periodic Trends

    2

    Big Idea: The structure of atomsmust be explainedusing quantummechanics, a theory in

    which the properties of

    particles and wavesmerge together.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Electromagnetic Radiation

    Electromagnetic Radiation:Consists of oscillating(time-varying)electric and magnetic fields thattravel through space at 2.998 108

    (c = speed

    of light) or just over 660 million mph.

    3

    Note All forms of radiation transfer energy from one region of space into another.

    Examples of Electromagnetic Radiation

    Visible light

    Radio Waves

    X-Rays

    Chapter 2: Quantum Mechanics and Atomic Theory

    Electromagnetic Radiation

    Wavelength (): Is thepeak-to-peak distance.

    Amplitude: Determinesbrightness of theradiation.

    Frequency (): Thenumber of cycles persecond (1 1

    ).

    4

    Note

    Changing the wavelength changes the

    region of the spectrum (i.e. x-ray to visible).

    Chapter 2: Quantum Mechanics and Atomic Theory

    Electromagnetic Radiation

    5Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    If white light is passedthrough a prism, acontinuous spectrumof light is found.However, when the

    light emitted byexcited hydrogenatoms is passedthrough a prism theradiation is found toconsist of a numberof components orspectra lines.

    6

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Black Body: An object that absorbs and emits allfrequencies of radiation without favor.

    Heated Black Bodies

    . .

    7

    Note max is the most prevalent wavelength, not the longest wavelength.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Theory

    Scientists used classical physics arguments toderive an expression for the energy density

    (Rayleigh Jens Law).

    The Problem With Explaining Black Body RadiationUsing Classical Mechanics

    Classical mechanics put

    no limits on minimum

    wavelength therefore at

    very small , would be a

    huge value even for low temperatures.

    8

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Max Plank: Proposed that the exchangeof energy between matter and radiationoccurs in quanta, or packets of energy.His central idea was that a chargedparticle oscillating at a frequency , canexchange energy with its surroundings bygenerating or absorbing electromagneticradiation only in discrete packets ofenergy.

    9

    Quanta: Packet of energy (implies minimumenergy that can be emitted).

    Charged particles oscillating at a frequency, ,can only exchange energy with theirsurroundings in discrete packets of energy.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Photoelectric Effect:Ejection of electrons from ametal when its surface is exposed to ultra violetradiation.

    10

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Findings of the Photoelectric Effect

    1) No electrons are ejected unless the radiation has afrequency above a certain threshold valuecharacteristic of the metal.

    2) Electrons are ejected immediately, however low theintensity of the radiation.

    3) The kinetic energy of the ejected electronsincreases linearly with the frequency of the incidentradiation.

    Albert Einstein

    Proposed that electromagnetic radiation consistsof massless particles (photons)

    Photons are packets of energy

    Energy of a single photon =

    11Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Photoelectric Effect Electromagnetic radiation consists of streams of photons

    traveling with frequency, , and energy .

    Photons collide with metal.

    If the photons have enough energy, electrons will be

    removed from the metal.

    Work Function ():The minimum amount ofenergy required to remove an electron from thesurface of a metal.

    If no electron ejected

    If electron will be ejected

    12

    Note This relationship is not intensity dependent.

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    With what speed will the fastest electronsbe emitted from a surface whose

    threshold wavelength is 600. nm, whenthe surface is illuminated with l ight ofwavelength 4.010

    7?

    13Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    H atoms only emit/absorb certainfrequencies.

    What is causing these properties?

    Electrons can only exist withcertain energies.

    The spectral lines are transitionsfrom one allowed energy level toanother.

    14

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Finding energy levels of H atom

    3.29 10

    (Found experimentally)

    3.29 10

    6.626 10

    3.29 10

    -2.178 10

    =

    Energ y leve l of H ato m

    2.178 10

    n= 1, 2, 3,

    Energ y level of othe r 1e-system s

    2.178 10

    n= 1, 2, 3,

    15

    Note In this equation n2 is always the large number which corresponds to the

    higher energy level.

    Note

    The negative sign appeared because a negative sign was taken out of

    parenthesis.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Student Question

    Quantum Theory

    What is the wavelength of the radiationemitted by a 2

    atom when an electron

    transitions between 4 to the 2 levels?

    Help ful Hint: c = 2.998108

    a ) -1.6641024m

    b ) -5.39910-8m

    c ) 1.62110-7m

    d ) 4.86410-7m

    e )None o f t he Above

    16

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    ConstructiveInterference: When thepeaks of wavescoincide, the amplitudeof the resulting wave is

    increased.

    Destructive Interference:When the peak of onewave coincides with thetrough of another wavethe resulting wave isdecreased.

    17Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    When light passes

    though a pair of closely

    spaced slits, circularwaves are generated at

    each slit. These waves

    interfere with each

    other.

    Where they interfereconstructively, a bright

    line is seen on the screen

    behind the slits; where

    the interference is

    destructive, the screen is

    dark.

    18

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Student Question

    Quantum Theory

    What is the wavelength of an electron travelingat

    the speed of light?

    Helpful informa t ion: 9.109 10 a n dh = 6.62610-34Js

    a ) 2.4210-9m

    b ) 2.4210-12m

    c ) 4.121011m

    d )None o f t he Above

    19Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Particles have wave like properties, therefore,classical mechanics are incorrect.

    Classical Mechanics:

    Particles have a defined trajectory.

    Location and linear momentum can bespecified at every moment.

    Quantum Mechanics:

    Particles behave like waves.

    Cannot specify the precise location of aparticle.

    20

    Note For the hydrogen atom, the duality means that we are not going to be able

    to know the speed of an electron orbiting the nucleus in a definite trajectory.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Theory

    Wavefunction ():A solution of the Schrdingerequation; the probability amplitude.

    Probability Density ():A function that, whenmultiplied by volume of the region, gives theprobability that the particle will be found in thatregion of space.

    21

    Note This gives you a representation of the particles trajectory.

    Examples

    sin

    Note This value must be between 0 and 1

    Chapter 2: Quantum Mechanics and Atomic Theory

    Particle in a Box

    Particle in a 1-D Box

    Boundary Conditions

    0 0

    0

    What is the wavefunction?

    sin sin0 0 sin 0

    22

    Note The term

    is there for normalization in order to get 1

    Note n is a quantum number. Quantum numbers are integers or integers

    that label a wavefunction.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Take 1st derivative of

    Take 2nd derivative of

    Particle in a Box

    Get the allowed energy levels from Schrdingers equation

    23

    What are the allowed energy levels?

    Note V(x)=0 for the particle in a box

    Chapter 2: Quantum Mechanics and Atomic Theory

    Particle in a Box

    Plug 2nd derivative back into wavefunction

    sin

    sin

    Cancel out

    Simplify

    24

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    Chapter 2: Quantum Mechanics and Atomic Theory

    The Hydrogen Atom

    Atomic Orbitals:A regionof space in which there isa high probability offinding an electron in an

    atom.

    The wavefunction of an electron is given inspherical polar coordinates

    = distance from the center of the atom

    = the angle from the positive z-axis, which can bethought of as playing the role of the geographicallatitude

    = the angle about the z-axis, the geographicallongitude

    25

    Note The wavefunctions of electrons

    are the atomic orbitals.

    Chapter 2: Quantum Mechanics and Atomic Theory

    The Hydrogen Atom

    Wavefunction of an electron in a1-electron atom

    ,, ,

    Radial Wavefunction

    , Angular Wavefunction

    26

    Chapter 2: Quantum Mechanics and Atomic Theory

    The Hydrogen Atom

    General wavefunction expression for a hydrogenatom:

    27

    +1

    -1

    0

    +2

    -1

    +1

    -2

    0

    Chapter 2: Quantum Mechanics and Atomic Theory

    The Hydrogen Atom

    Schrdinger Equation for the H-atom

    sin

    Columbic potential energy between the protonand electron

    Reduced mass (proton and electron)

    Scientists have solved for the energy of the H-atom

    .

    3.290 10

    principle quantum number can be 1, 2, 3,

    planks constant 6.6260810-34Js

    28

    Chapter 2: Quantum Mechanics and Atomic Theory

    The Hydrogen Atom

    Pictured: Thepermitted energylevels of ahydrogen atom.

    The levels arelabeled with thequantum number which rangesfrom 1 (groundstate) to .

    29Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Numbers

    Principle Quantum Number

    Rela ted To: Size and Energy

    Al low ed Values: 1,2,3, (shells)

    30

    Note The larger the , the larger the size, the larger the orbital, and the larger theenergy.

    Note When identifying the orbital, the value comes in front of the orbital type.

    Example

    3p 3

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Numbers

    Angular MomentumQuantum Number ()

    Relate d To:Shape

    Al low ed Values: 0,1,2, , 1 (subshells)

    What are the possible valuesgiven the following values?

    1 1

    2 2

    3 3

    What type of orbital is associated withthe following quantum numbers?

    1 1 and 0

    2 2 and 13 3 and 0

    31

    Valueof l

    OrbitalType

    0 s

    1 p

    2 d

    3 f

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Numbers

    Magnetic Quantum Number ()

    Rela te d To: Orientation in space

    (specifies exactly which orbital [ex: ])Al low ed Va lues: , 1, ,0 , , (orbitals)

    What are the possible values of given thefollowing and values:

    1 1 and 0

    2 2 and 1

    3 2 and 0

    32

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Numbers

    33

    Note The quantum number ml is an alternative label for the individual orbitals: inchemistry, it is more common to use x, y, and z instead.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Numbers

    A summary of the arrangements of shells,subshells, and orbitals in an atom and the

    corresponding quantum numbers.

    34

    Chapter 2: Quantum Mechanics and Atomic Theory

    Student Question

    Quantum Numbers

    The following set of quantum numbers is notallowed: 3, 0, 2. Assuming thatthe and values are correct, change the value to an allowable combination.

    a) 1

    b) 2

    c) 3

    d) 4

    e) None of the Above

    35Chapter 2: Quantum Mechanics and Atomic Theory

    Quantum Numbers

    Electron Spin Quantum Number()

    Rela te d To:Spin of the electron

    Al low ed Va lues: (spin up ) or - (spindown )

    36

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Orbitals

    What does an s-orbital ( 0) look like?

    1 and 0

    (radial wavefunction)

    ,

    (angular wavefuction)

    , ,

    , ,

    37Chapter 2: Quantum Mechanics and Atomic Theory

    Orbitals

    The three s-orbitals ( ) of lowest energy

    The simplest way ofdrawing an atomic

    orbital is as a boundarysurface, a surface within which there is a high probability

    (typically 90%) of finding the electron. The darker theshaded region within the boundary surfaces, the larger the

    probability of the electron being found there.

    38

    Chapter 2: Quantum Mechanics and Atomic Theory

    Orbitals

    What do p-orbitals ( 1) look like?

    39Chapter 2: Quantum Mechanics and Atomic Theory

    Orbitals

    What do d-orbitals ( 2) look like?

    40

    Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    The electrons in many-electron atomsoccupy orbitals like those of hydrogenbut the energy of the orbitals differ.

    Differences between the many-electronorbital energies and hydrogen atomorbital energies:

    The nucleus of the many-electron orbitals havemore positive charge attracting the electrons,thus lowering the energy.

    The electrons repel each other raising theenergy.

    41Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    The number of electrons in an atom affects theproperties of the atom.

    42

    Note H with 1 electron has no electron-electron repulsion and the electron will have

    the same energy if is the 2s or 2p orbital (all orbitals within one shell degenerate).

    Potential Energy for He atom (2 p and 2 e-)

    Attraction of

    electron 1 to

    the nucleus

    Attraction of

    electron 2 to

    the nucleus

    Repulsion

    between the

    two electrons

    2

    4

    2

    4

    4

    1 = distance between electron 1 and the nucleus

    2 = distance between electron 2 and the nucleus

    12 = distance between the two electrons

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    Why do the energies change?

    Shielding: The repulsion experienced byan electron in an atom that arises from

    the other electrons present andopposes the attraction exerted by thenucleus.

    Effective Nuclear Charge (Zeff):The netnuclear charge after taking intoaccount the shielding caused by otherelectrons in the atom.

    43

    Amount of Shielding

    Distance from nucleus

    Note s electrons can penetrate through the nucleus while p and

    d electrons cannot.

    S P D F

    Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    44

    Order of Orbital Filling

    1s 2s 2p 3s 3p 4s 3d 4p 5s 4d 5p

    7s 7p 7d 7f

    6s 6p 6d 6f

    5s 5p 5d 5f

    4s 4p 4d 4f

    3s 3p 3d

    2s 2p

    1s

    Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    Electron Configuration: A list of an atomsoccupied orbitals with the number of electronsthat each contains.

    In the ground state the electrons occupy atomic orbitals

    in such a way that the total energy of the atom is aminimum.

    We might expect that atoms would have all their

    electrons in the 1s orbital however this is only true for Hand He.

    Pauli Exclusion Principle: No more than twoelectrons may occupy any given orbital. Whentwo electrons occupy one orbital, the spins mustbe paired.

    45

    Note Paired spins means and electron ()

    Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    Writing Electron Configurations

    Step 1:Determine the number of electrons theatom has.

    Step 2: Fill atomic orbitals starting with lowestenergy orbitals first and proceeding to higherenergy orbitals.

    Step 3:Determine how electrons fill the orbitals.

    46

    Subshell lSmallest

    ns 0 1p 1 2d 2 3f 3 4

    Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    Electron Configurations: He Step 1:

    Step 2:

    Step 3:

    Be Step 1:

    Step 2:

    Step 3:

    47Chapter 2: Quantum Mechanics and Atomic Theory

    Many Electron Atoms

    Electron Configurations: C Step 1:

    Step 2:

    Step 3: __ __ __ 2p __ __ __ 2p __ __ __ 2p

    2s 2s 2s

    1s 1s 1s

    48

    Note Electrons that are farther apart repel each other less.

    Note Electrons with parallel spins tend to avoid each other more.

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Periodic Trends

    Effective NuclearCharge:(Zeff) The netnuclear charge aftertaking into accountthe shielding causedby other electrons inthe atom.

    Why:Going across the periodic table, the numberof core electrons stays the same but the number

    of protons increases. The core electrons are

    responsible for most of the shielding, therefore the

    Zeff gets larger as you go across a period.

    Although going down a group adds more coreelectrons it also adds more protons therefore Zeff is

    pretty much constant going down a group.

    49Chapter 2: Quantum Mechanics and Atomic Theory

    Periodic Trends

    Atomic Radii:Half the distancebetween the centers

    of neighboring atomsin a solid of ahomonuclearmolecule.

    Why:Going across a period the Zeff increases,therefore the pull on the electrons increases andthe atomic radii decrease. Going down a group,

    more atomic shells are added and the radii

    increase.

    50

    Chapter 2: Quantum Mechanics and Atomic Theory

    Periodic Trends

    First Ionization Energy:The minimum energyrequired to remove thefirst electron from theground state of agaseous atom,molecule, or ion.

    X(g) X+(g) +e-

    Why:Going across a period the Zeff increasestherefore it is harder to remove an electron and

    the first ionization energy increases. However,

    going down a group the electrons are located

    farther from the nucleus and they can be

    removed easier.

    51Chapter 2: Quantum Mechanics and Atomic Theory

    Periodic Trends

    1st Ionization Energy Data

    Why dont B and Al fit the 1st ionization energy trend?

    52

    H

    He

    Li

    BeB

    C

    NO

    F

    Ne

    Na

    MgAl

    Si

    P S

    Cl

    Ar

    KCa

    0

    500

    1000

    1500

    2000

    2500

    0 1 2 3 4 5 6 7 8 9 1 0 11 12 13 14 15 16 17 18 19 20

    Ionizationenergy,kJmol-1

    Atomic Number

    Ionization Energies of the First 20 Elements

    Chapter 2: Quantum Mechanics and Atomic Theory

    Periodic Trends

    Electron Affinity: (Eea)The energy releasedwhen an electron isadded to agas-phase atom.

    X(g) + e- X-(g)

    Why:Going across a period the Zeff increasestherefore the atom has a larger positive charge

    and releases more energy when an electron is

    added to the atom. Going down a group theelectron is added farther from the nucleus and the

    electron affinity decreases. This trend does not holdtrue for the noble gases.

    53

    Note This trends has the most atoms that do not obey it.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Periodic Trends

    54

    H

    He

    Li

    BeB

    C

    N

    O

    F

    Ne

    Na

    Mg

    Al

    Si

    P

    S

    Cl

    Ar

    K

    Ca

    -50

    0

    50

    100

    150

    200

    250

    300

    350

    400

    0 1 2 3 4 5 6 7 8 9 1 0 11 12 13 14 15 16 17 18 19 20

    EA(kJ/mole)

    Atomic Number

    Electron Affinity of the First 20 Elements

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    Chapter 2: Quantum Mechanics and Atomic Theory

    Take Away From Chapter 12

    Big Idea: The structure of atoms must be explainedusing quantum mechanics, a theory in which theproperties of particles and waves merge together.

    Electromagnetic Radiation (22)

    Be able to change between frequency and wavelength

    Be able to assign what area of the electromagneticspectrum radiation comes from.

    55

    Numbers correspond to end of chapter questions.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Take Away From Chapter 12

    Quantum Theory

    Know that electromagnetic radiation has both wave andmatter properties. (30)

    Photo electric effect (particle property) (27, 28, 29)

    Know what the work function of a material is Diffraction (wave property)

    Be able to calculate the energy carried in an

    electromagnetic wave (21, 25)

    Know that matter has both wave and matter properties.

    Be able to calculate the wavelength of matter. (32, 34, 35)

    Know that the Heisenberg uncertainty principle determines

    the accuracy in which we can measure momentum andposition.

    56

    Numbers correspond to end of chapter questions.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Take Away From Chapter 12

    Particle in a Box

    Know that the wavefunction of different systems can be

    found using boundary conditions.

    Particle in a box wavefunction

    sin

    Know that the square of the wavefunction tells us the

    probability of the particle being in a certain location

    Know the most likely location of a particle in a box (ex: n = 1

    particle most likely in center of box, n = 2 particle most likely onsides of box)

    Know that the Schrdinger equation allows us to matchwavefunctions with allowed energy values.

    Particle in a box

    (53, 54, 55, 57)

    The Hydrogen Atom

    Know that when quantum mechanics is applied to 1

    electron systems the observed energy and the theoretical

    energies match. (38, 40, 41, 42, 44, 46, 47, 141) 2.178 10

    57

    Numbers correspond to end of chapter questions.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Take Away From Chapter 12

    Quantum Number (58,62,64,65,66, 74,75) Know that the quantum number gives the size and

    energy

    Allowed values of 1,2,

    Know that the quantum number l gives the orbital type(shape)

    Allowed values of 0 ,1 ,2 , 1

    Know that the quantum number gives the orbitalorientation (ex: ) Allowed values of ,0,

    Know that a fourth quantum number was needed to have theory

    match experiment, Allowed values of

    58

    Numbers correspond to end of chapter questions.

    Chapter 2: Quantum Mechanics and Atomic Theory

    Take Away From Chapter 12

    Orbitals Know that when atomic orbitals are drawn they represent the

    area in which e- have a 90% chance of being in. (67)

    Know the what s, p, and d orbitals look like.

    Many Electron Atoms

    Be able to write both the full and shorthand electronconfigurations of atoms.(76, 77, 80, 84, 92)

    Be able to predict the number of unpaired electrons in asystem.(90, 91)

    Periodic Trends Know the trends of effective nuclear charge, atomic radii,

    ionization energy, and electron affinity. (13, 14, 96, 97, 98, 100, 106,

    111, 112, 133, 136)

    59

    Numbers correspond to end of chapter questions.