Chapter 6 Lecture- Electrons in Atoms

91
Waves To understand the electronic structure of atoms, one must understand the nature of electromagnetic radiation. The distance between corresponding points on adjacent waves is the wavelength ().

description

Chapter 6 Lecture for AP Chemistry

Transcript of Chapter 6 Lecture- Electrons in Atoms

Page 1: Chapter 6 Lecture- Electrons in Atoms

Waves

• To understand the electronic structure of atoms, one must understand the nature of electromagnetic radiation.

• The distance between corresponding points on adjacent waves is the wavelength ().

Page 2: Chapter 6 Lecture- Electrons in Atoms

Waves• The number of waves

passing a given point per unit of time is the frequency ().

• For waves traveling at the same velocity, the longer the wavelength, the smaller the frequency.

Page 3: Chapter 6 Lecture- Electrons in Atoms

Electromagnetic Radiation

• All electromagnetic radiation travels at the same velocity: the speed of light (c), 3.00 108 m/s.

• Therefore,

c =

Page 4: Chapter 6 Lecture- Electrons in Atoms

Visible light is only one form of electromagnetic radiation; all visible light is electromagnetic radiation, but not all electromagnetic radiation is visible light.

Page 5: Chapter 6 Lecture- Electrons in Atoms

Both visible light and X rays travel at the same speed, about 186,000 miles per second.

Page 6: Chapter 6 Lecture- Electrons in Atoms

SAMPLE EXERCISE 6.1 Concepts of Wavelength and Frequency

Two electromagnetic waves are represented in the image below. (a) Which wave has the higher frequency? (b) If one wave represents visible light and the other represents infrared radiation, which wave is which?

(b) The electromagnetic spectrum (Figure 6.4) indicates that infrared radiation has a longer wavelength than visible light. Thus, the lower wave would be the infrared radiation.

Solution (a) The lower wave has a longer wavelength (greater distance between peaks). The longer the wavelength, the lower the frequency ( = c/ ). Thus, the lower wave has the lower frequency, and the upper one has the higher frequency.

Page 7: Chapter 6 Lecture- Electrons in Atoms

Answer: The expanded visible-light portion of Figure 6.4 tells you that red light has a longer wavelength than blue light. The lower wave has the longer wavelength (lower frequency) and would be the red light.

PRACTICE EXERCISE

If one of the waves in the image above represents blue light and the other red light, which is which?

Page 8: Chapter 6 Lecture- Electrons in Atoms

SAMPLE EXERCISE 6.2 Calculating Frequency from Wavelength

The yellow light given off by a sodium vapor lamp used for public lighting has a wavelength of 589 nm. What is the frequency of this radiation?

Solve: Solving Equation 6.1 for frequency gives = c/ . When we insert the values for c and , we note that the units of length in these two quantities are different. We can convert the wavelength from nanometers to meters, so the units cancel:

Check: The high frequency is reasonable because of the short wavelength. The units are proper because frequency has units of “per second,” or s–1.

Page 9: Chapter 6 Lecture- Electrons in Atoms

PRACTICE EXERCISE

(a) A laser used in eye surgery to fuse detached retinas produces radiation with a wavelength of 640.0 nm. Calculate the frequency of this radiation. (b) An FM radio station broadcasts electromagnetic radiation at a frequency of 103.4 MHz (megahertz; MHz = 106 s–1). Calculate the wavelength of this radiation.

Answers: (a) 4.688 1014 s–1, (b) 2.901 m

Page 10: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy• The wave nature of light

does not explain how an object can glow when its temperature increases.

• Max Planck explained it by assuming that energy comes in packets called quanta.

Page 11: Chapter 6 Lecture- Electrons in Atoms

As temperature increases, the average energy of the emitted radiation increases. Blue-white light is at the shorter wavelength (higher energy) end of the visible spectrum while red light is at the longer wavelength (lower energy) end of the visible spectrum.

Page 12: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy

• Einstein used this assumption to explain the photoelectric effect.

• He concluded that energy is proportional to frequency:

E = hwhere h is Planck’s constant, 6.63 10−34 J-s.

Page 13: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy

• Therefore, if one knows the wavelength of light, one can calculate the energy in one photon, or packet, of that light:

c = E = h

Page 14: Chapter 6 Lecture- Electrons in Atoms

SAMPLE EXERCISE 6.3 Energy of a Photon

Calculate the energy of one photon of yellow light whose wavelength is 589 nm.

This is the magnitude of enthalpies of reactions (Section 5.4), so radiation can break chemical bonds, producing what are called photochemical reactions.

Plan: We can use Equation 6.1 to convert the wavelength to frequency:

We can then use Equation 6.3 to calculate energy:

Solve: The frequency, , is calculated from the given wavelength.

The value of Planck’s constant, h, is given both in the text and in the table of physical constants on the inside front cover of the text, and so we can easily calculate E:

Comment: If one photon of radiant energy supplies 3.37 10–19J, then one mole of these photons will supply

Page 15: Chapter 6 Lecture- Electrons in Atoms

SAMPLE EXERCISE 6.3 continued

Answers: (a) 3.11 10–19 J, (b) 0.16 J, (c) 4.2 1016 photons

PRACTICE EXERCISE(a) A laser emits light with a frequency of 4.69 1014 s–1. What is the energy of one photon of the radiation from this laser? (b) If the laser emits a pulse of energy containing 5.0 1017 photons of this radiation, what is the total energy of that pulse? (c) If the laser emits 1.3 10–2 J of energy during a pulse, how many photons are emitted during the pulse?

Page 16: Chapter 6 Lecture- Electrons in Atoms

Electrons would be ejected, and they would have greater kinetic energy than those ejected by yellow light.

Page 17: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy

Another mystery involved the emission spectra observed from energy emitted by atoms and molecules.

Page 18: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy

• One does not observe a continuous spectrum, as one gets from a white light source.

• Only a line spectrum of discrete wavelengths is observed.

Page 19: Chapter 6 Lecture- Electrons in Atoms

Photons of only certain allowed frequencies can be absorbed or emitted as the electron changes energy state.

Page 20: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy

• Niels Bohr adopted Planck’s assumption and explained these phenomena in this way:1. Electrons in an atom can only

occupy certain orbits (corresponding to certain energies).

Page 21: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy

• Niels Bohr adopted Planck’s assumption and explained these phenomena in this way:2. Electrons in permitted orbits

have specific, “allowed” energies; these energies will not be radiated from the atom.

Page 22: Chapter 6 Lecture- Electrons in Atoms

The Nature of Energy

• Niels Bohr adopted Planck’s assumption and explained these phenomena in this way:3. Energy is only absorbed or

emitted in such a way as to move an electron from one “allowed” energy state to another; the energy is defined by

E = h

Page 23: Chapter 6 Lecture- Electrons in Atoms

The Nature of EnergyThe energy absorbed or emitted from the process of electron promotion or demotion can be calculated by the equation:

E = −RH ( )1nf

2

1ni

2-

where RH is the Rydberg constant, 2.18 10−18 J, and ni and nf are the initial and final energy levels of the electron.

Page 24: Chapter 6 Lecture- Electrons in Atoms

SAMPLE EXERCISE 6.4 Electronic Transitions in the Hydrogen Atom

Using Figure 6.13, predict which of the following electronic transitions produces the spectral line having the longest wavelength: n = 2 to n = 1, n = 3 to n = 2, or n = 4 to n = 3.

Solution The wavelength increases as frequency decreases ( = c/. Hence the longest wavelength will be associated with the lowest frequency. According to Planck’s equation, E = h, the lowest frequency is associated with the lowest energy. In Figure 6.13 the shortest vertical line represents the smallest energy change. Thus, the n = 4 to n = 3 transition produces the longest wavelength (lowest frequency) line.

Page 25: Chapter 6 Lecture- Electrons in Atoms

Answers: (a) emits energy, (b) requires absorption of energy

PRACTICE EXERCISEIndicate whether each of the following electronic transitions emits energy or requires the absorption of energy: (a) n = 3 to n = 1; (b) n = 2 to n = 4 .

Page 26: Chapter 6 Lecture- Electrons in Atoms

It absorbs energy.

Page 27: Chapter 6 Lecture- Electrons in Atoms

Considering only the n = 1 to n = 5 states in the hydrogen atom, which transition will emit

the most energy?

• n = 5 to n = 4• n = 5 to n = 2• n = 3 to n = 1• n = 3 to n = 2• n = 4 to n = 2

Page 28: Chapter 6 Lecture- Electrons in Atoms

• n = 5 to n = 4• n = 5 to n = 2• n = 3 to n = 1• n = 3 to n = 2• n = 4 to n = 2

Considering only the n = 1 to n = 5 states in the hydrogen atom, which transition will emit

the most energy?

Page 29: Chapter 6 Lecture- Electrons in Atoms

Considering only the n = 1 to n = 5 states in the hydrogen atom, which transition will emit

the longest wavelength?

• n = 5 to n = 4

• n = 5 to n = 2

• n = 3 to n = 1

• n = 3 to n = 2

• n = 4 to n = 2

Page 30: Chapter 6 Lecture- Electrons in Atoms

• n = 5 to n = 4

• n = 5 to n = 2

• n = 3 to n = 1

• n = 3 to n = 2

• n = 4 to n = 2

Considering only the n = 1 to n = 5 states in the hydrogen atom, which transition will emit

the longest wavelength?

Page 31: Chapter 6 Lecture- Electrons in Atoms

What is the wavelength for radiation transmitted by WGR, 550 AM (550 kHz)?

1. 0.545 m2. 5.45 m3. 545 m4. 0.0018 m5. 1.8 m

Page 32: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. 0.545 m2. 5.45 m3. 545 m4. 0.0018 m5. 1.8 m

)s10(5.5

)ms10(3.015

18

c

545=

Page 33: Chapter 6 Lecture- Electrons in Atoms

Predict which of the following electronic transitions will produce the longest wavelengthspectral line.

1. n = 4 to n = 22. n = 5 to n = 23. n = 5 to n = 34. n = 6 to n = 4

Page 34: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. n = 4 to n = 22. n = 5 to n = 23. n = 5 to n = 34. n = 6 to n = 4

The wavelength increases as frequency decreases. The lowest frequency (longest wavelength) is associated with the lowest energy, and the smallest energy difference here is between n = 6 and n = 4.

Page 35: Chapter 6 Lecture- Electrons in Atoms

Observations that led to the development of quantum mechanics

1. Hot objects emit electromagnetic radiation. (blackbody radiation)

2. Metals eject electrons when struck by a minimum frequency/energy of electromagnetic radiation.(the photoelectric effect)

3. Excited atoms emit electromagnetic radiation of certain frequencies. (atomic emission spectra)

Bellwork- The Photoelectric Effect

A photon with a minimum energy of 4.41x10-19J will cause emission of an electron from sodium metal.

a)What frequency and wavelength of light does this correspond to?

b)What type of light is it?

c)Describe what happens if yellow light hits sodium metal.

d)Describe what happens when UV light irradiates Na(s)

E=hv v=6.66x1014s-1

c=λν λ=4.50x10-7m λ=450nm

Visible, turquoise!

Sodium electrons may absorb some photons/energy, but it is not enough to help the e- escape

Sodium electrons may absorb some photons, and then they will have more than enough energy to escape (n= ∞). The electron is FREE! Extra energy = KE.

Page 36: Chapter 6 Lecture- Electrons in Atoms

The Wave Nature of Matter

• Louis de Broglie posited that if light can have material properties, matter should exhibit wave properties.

• He demonstrated that the relationship between mass and wavelength was

=h

mv

Page 37: Chapter 6 Lecture- Electrons in Atoms

The Uncertainty Principle

• Heisenberg showed that the more precisely the momentum of a particle is known, the less precisely is its position known:

• In many cases, our uncertainty of the whereabouts of an electron is greater than the size of the atom itself!

(x) (mv) h4

Page 38: Chapter 6 Lecture- Electrons in Atoms

Quantum Mechanics

• Erwin Schrödinger developed a mathematical treatment into which both the wave and particle nature of matter could be incorporated.

• It is known as quantum mechanics.

Page 39: Chapter 6 Lecture- Electrons in Atoms

Quantum Mechanics

• The wave equation is designated with a lower case Greek psi ().

• The square of the wave equation, 2, gives a probability density map of where an electron has a certain statistical likelihood of being at any given instant in time.

Page 40: Chapter 6 Lecture- Electrons in Atoms

Quantum Numbers

• Solving the wave equation gives a set of wave functions, or orbitals, and their corresponding energies.

• Each orbital describes a spatial distribution of electron density.

• An orbital is described by a set of three quantum numbers.

Page 41: Chapter 6 Lecture- Electrons in Atoms

Principal Quantum Number, n

• The principal quantum number, n, describes the energy level on which the orbital resides.

• The values of n are integers ≥ 0.

Page 42: Chapter 6 Lecture- Electrons in Atoms

Azimuthal Quantum Number, l

• This quantum number defines the shape of the orbital.

• Allowed values of l are integers ranging from 0 to n − 1.

• We use letter designations to communicate the different values of l and, therefore, the shapes and types of orbitals.

Page 43: Chapter 6 Lecture- Electrons in Atoms

Azimuthal Quantum Number, l

Value of l 0 1 2 3

Type of orbital s p d f

Page 44: Chapter 6 Lecture- Electrons in Atoms

Magnetic Quantum Number, ml

• Describes the three-dimensional orientation of the orbital.

• Values are integers ranging from -l to l:

−l ≤ ml ≤ l.

• Therefore, on any given energy level, there can be up to 1 s orbital, 3 p orbitals, 5 d orbitals, 7 f orbitals, etc.

Page 45: Chapter 6 Lecture- Electrons in Atoms

Magnetic Quantum Number, ml

• Orbitals with the same value of n form a shell.• Different orbital types within a shell are

subshells.

Page 46: Chapter 6 Lecture- Electrons in Atoms

s Orbitals

• Value of l = 0.• Spherical in shape.• Radius of sphere

increases with increasing value of n.

Page 47: Chapter 6 Lecture- Electrons in Atoms

s Orbitals

Observing a graph of probabilities of finding an electron versus distance from the nucleus, we see that s orbitals possess n−1 nodes, or regions where there is 0 probability of finding an electron.

Page 48: Chapter 6 Lecture- Electrons in Atoms

p Orbitals

• Value of l = 1.• Have two lobes with a node between them.

Page 49: Chapter 6 Lecture- Electrons in Atoms

d Orbitals• Value of l is 2.• Four of the five

orbitals have 4 lobes; the other resembles a p orbital with a doughnut around the center.

Page 50: Chapter 6 Lecture- Electrons in Atoms

What is the maximum number of orbitals described by the quantum numbers:

• 1• 3• 5• 8• 9

n = 3 l = 2

Page 51: Chapter 6 Lecture- Electrons in Atoms

What is the maximum number of orbitals described by the quantum numbers:

• 1• 3• 5• 8• 9

n = 3 l = 2

Page 52: Chapter 6 Lecture- Electrons in Atoms

What is the maximum number of electrons described by the quantum number:

• 7• 14• 16• 32• 48

n = 4

Page 53: Chapter 6 Lecture- Electrons in Atoms

How many nodal planes does a d orbital have?

• 0• 1• 2• 3• 4

Page 54: Chapter 6 Lecture- Electrons in Atoms

How many nodal planes does a d orbital have?

• 0• 1• 2• 3• 4

Page 55: Chapter 6 Lecture- Electrons in Atoms

Which of the following is not an allowed set of quantum numbers?

1. n = 3, l = 1, ml = 1

2. n = 3, l = 3, ml =23. n = 4, l = 0, ml = 0

4. n = 3, l = 1, ml =1

Page 56: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. n = 3, l = 1, ml = 1

2. n = 3, l = 3, ml =23. n = 4, l = 0, ml = 0

4. n = 3, l = 1, ml =1

The value of l can be no larger than n 1.

Page 57: Chapter 6 Lecture- Electrons in Atoms

How many electrons maximum can exist in the 4d orbital?

1. 2 2. 63. 104. 14

Page 58: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. 2 2. 63. 104. 14

There are five 4d orbitals, each of which can contain up to 2 electrons each for a total of 10 maximum.

Page 59: Chapter 6 Lecture- Electrons in Atoms

The electron subshell 3p represents the principal quantum number n = ___ and azimuthal quantum number l = ___.

1. 3; 2 2. 2; 33. 3; 14. 1; 3

Page 60: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. 3; 2 2. 2; 33. 3; 14. 1; 3

The principal quantum number n is 3, and a p orbital indicates l = 1.

Page 61: Chapter 6 Lecture- Electrons in Atoms

The maximum number of electrons in an atom that can exist in the 4f subshell and have ml = 1 is

1. 2 2. 73. 144. 32

Page 62: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. 2 2. 73. 144. 32

For any value of ml, the maximum number of electrons is 2.

Page 63: Chapter 6 Lecture- Electrons in Atoms

Energies of Orbitals

• For a one-electron hydrogen atom, orbitals on the same energy level have the same energy.

• That is, they are degenerate.

Page 64: Chapter 6 Lecture- Electrons in Atoms

Energies of Orbitals

• As the number of electrons increases, though, so does the repulsion between them.

• Therefore, in many-electron atoms, orbitals on the same energy level are no longer degenerate.

Page 65: Chapter 6 Lecture- Electrons in Atoms

Spin Quantum Number, ms

• In the 1920s, it was discovered that two electrons in the same orbital do not have exactly the same energy.

• The “spin” of an electron describes its magnetic field, which affects its energy.

Page 66: Chapter 6 Lecture- Electrons in Atoms

Spin Quantum Number, ms

• This led to a fourth quantum number, the spin quantum number, ms.

• The spin quantum number has only 2 allowed values: +1/2 and −1/2.

Page 67: Chapter 6 Lecture- Electrons in Atoms

Pauli Exclusion Principle

• No two electrons in the same atom can have exactly the same energy.

• For example, no two electrons in the same atom can have identical sets of quantum numbers.

Page 68: Chapter 6 Lecture- Electrons in Atoms

Electron Configurations

• Distribution of all electrons in an atom.

• Consist of Number denoting the

energy level

Page 69: Chapter 6 Lecture- Electrons in Atoms

Electron Configurations

• Distribution of all electrons in an atom.

• Consist of Number denoting the

energy levelLetter denoting the type

of orbital.

Page 70: Chapter 6 Lecture- Electrons in Atoms

Electron Configurations

• Distribution of all electrons in an atom.

• Consist of Number denoting the

energy level.Letter denoting the type

of orbital.Superscript denoting the

number of electrons in those orbitals.

Page 71: Chapter 6 Lecture- Electrons in Atoms

QuickTime™ and aSorenson Video decompressorare needed to see this picture.

Page 72: Chapter 6 Lecture- Electrons in Atoms

Orbital Diagrams

• Each box represents one orbital.

• Half-arrows represent the electrons.

• The direction of the arrow represents the spin of the electron.

Page 73: Chapter 6 Lecture- Electrons in Atoms

Hund’s Rule

“For degenerate orbitals, the lowest energy is attained when the number of electrons with the same spin is maximized.”

Page 74: Chapter 6 Lecture- Electrons in Atoms

Periodic Table

• We fill orbitals in increasing order of energy.

• Different blocks on the periodic table, then correspond to different types of orbitals.

Page 75: Chapter 6 Lecture- Electrons in Atoms

What are the valence electrons of vanadium?

• 4s2

• 3d3

• 4s2 3d3

• 3d5

• 4d5

Page 76: Chapter 6 Lecture- Electrons in Atoms

What are the valence electrons of vanadium?

• 4s2

• 3d3

• 4s2 3d3

• 3d5

• 4d5

Page 77: Chapter 6 Lecture- Electrons in Atoms

What are the valence electrons of gallium?

• 4s2

• 4p1

• 4s2 3d10 4p1

• 4s2 3d10

• 4s2 4p1

Page 78: Chapter 6 Lecture- Electrons in Atoms

What are the valence electrons of gallium?

• 4s2

• 4p1

• 4s2 3d10 4p1

• 4s2 3d10

• 4s2 4p1

Page 79: Chapter 6 Lecture- Electrons in Atoms

How many unpaired electrons does selenium have?

• 0• 2• 4• 6• 8

Page 80: Chapter 6 Lecture- Electrons in Atoms

How many unpaired electrons does selenium have?

• 0• 2• 4• 6• 8

Page 81: Chapter 6 Lecture- Electrons in Atoms

The following orbital diagram represents the electron configuration of which element?

1. Carbon2. Nitrogen3. Oxygen4. Neon

1s 2s 2p

Page 82: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. Carbon2. Nitrogen3. Oxygen4. Neon

1s 2s 2p

Page 83: Chapter 6 Lecture- Electrons in Atoms

What is the characteristic outer shell electron configuration of the noble gases?

1. s2p6

2. s2p5

3. s2p4

4. s2p3

Page 84: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1. s2p6

2. s2p5

3. s2p4

4. s2p3

Noble gases have completely filled s and p orbitals, hence their lack of reactivity.

Page 85: Chapter 6 Lecture- Electrons in Atoms

Some Anomalies

Some irregularities occur when there are enough electrons to half-fill s and d orbitals on a given row.

Page 86: Chapter 6 Lecture- Electrons in Atoms

Some Anomalies

For instance, the electron configuration for copper is

[Ar] 4s1 3d5

rather than the expected

[Ar] 4s2 3d4.

Page 87: Chapter 6 Lecture- Electrons in Atoms

Some Anomalies

• This occurs because the 4s and 3d orbitals are very close in energy.

• These anomalies occur in f-block atoms, as well.

Page 88: Chapter 6 Lecture- Electrons in Atoms

How many unpaired electrons does chromium have?

• 0• 2• 4• 6• 8

Page 89: Chapter 6 Lecture- Electrons in Atoms

How many unpaired electrons does chromium have?

• 0• 2• 4• 6• 8

Page 90: Chapter 6 Lecture- Electrons in Atoms

Which of the following orbital diagrams obeys Hund’s rule for a ground-state atom?1.

2.

3.

3s 3d

3s 3d

3s 3d

Page 91: Chapter 6 Lecture- Electrons in Atoms

Correct Answer:

1.

2.

3.

3s 3d

3s 3d

3s 3d