lecture 21 & 22...orbital shape magnetic m l integers from -l to 0 to +l orbital orientation...

53
ANNOUNCEMENTS Chapter 5 homework due Friday March 6. Chapter 6 homework due Friday March 13. Quiz 2 due Thursday March 12 and Exam 2 is March 14. Review the exam (learn from your mistakes) Go to the help room GMCS-212 Go to the Supplemental Instruction sessions

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Page 1: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ANNOUNCEMENTS• Chapter 5 homework due Friday March 6.

• Chapter 6 homework due Friday March 13.

• Quiz 2 due Thursday March 12 and Exam 2 is March 14.

• Review the exam (learn from your mistakes)

• Go to the help room GMCS-212

• Go to the Supplemental Instruction sessions

Page 2: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUANTUM NUMBERS1

0

0

2 3

0 1 0 1 2

-1,0,1

2p1s

0

2s

-1,0,1

3p

0

3s

-2,-1,0,1,2

3d

Principal: n(size, energy)

Angular momentum: l

(shape)

Magnetic: ml

(orientation)

Orbital:

Page 3: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

NAMING ATOMIC ORBITALS• An atomic orbital is designated by its value for n (level)

and l (sublevel).

• In naming, the level (n value) is used directly, the sublevel (l value) is expressed as a letter :

• l = 0 - s (sharp)

• l = 1 - p (principal)

• l = 2 - d (diffuse)

• l = 3 - f (fundamental)

Page 4: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

PROBLEMThe set of quantum numbers below is not allowed.

Assuming that both the n and ml values are correct, what value should l be in order for the quantum number to be

allowable?n = 3, l = 0, ml = -2

(a) l = 1 (b) l = 2(c) l = 4(d) l = -1(e) l = -2

Page 5: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

1s 2s 3s

1s: n = 1 , l = 0, ml = 0

Page 6: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

2P ATOMIC ORBITAL

n = 2 , l = 1, ml = -1, 0, 1

Page 7: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

3D ATOMIC ORBITALn = 3 , l = 2, ml = -2, -1, 0, 1, 2

Page 8: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

4F ORBITAL

This is one of the seven different f orbitals.

The larger orbitals are more complex with more lobes and

nodes in their structure.

Page 9: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ORBITAL NAMING

• n = 2 , l = 0

• n = 3 , l = 1

• n = 4 , ml = +3

• n = 2 , l = 1

What are the names of these orbitals?

Page 10: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

HYDROGEN ATOM BEAM• Hydrogen atoms have one proton and one electron.

• Every hydrogen atom should be the same.

• Pass a beam of H atoms through a magnetic field and the atoms separate into two paths.

Page 11: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

SUMMARY OF QUANTUM NUMBERS OF ELECTRONS IN ATOMS

Name Symbol Permitted Values Property

principal n Positive integers (1,2,3...)

Orbital energy (size)

angular momentum l Integers from 0

to n-1 Orbital shape

magnetic mlIntegers from -l

to 0 to +lOrbital

orientation

spin ms +½ or -½ Direction of e- spin

Spin up = +½ ↑Spin down = -½ ↓

Two e- per orbital: ↑↓spin paired

Page 12: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUANTUM NUMBERS & ELECTRONS

1

0

0

2 3

0 1 0 1 2

-1,0,10 -1,0,10 -2,-1,0,1,2

Principal: n(size, energy)

Angular momentum: l

(shape)

Magnetic: ml

(orientation)

Electrons: 2e- 2e- 2e-6e- 6e- 10e-

Page 13: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

PAULI EXCLUSION PRINCIPLE• Two electrons that are in the same atom cannot have the

same set of quantum numbers.

• Each electron in an atom must have its own unique set of quantum numbers (its own unique identity)

• Allowed configuration - abides by the Exclusion Principle

• Forbidden configuration - violates the Exclusion Principle

Page 14: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

WHAT IS THE GROUND STATE CONFIGURATION FOR HELIUM?Ground state electron configuration for hydrogen:

H = 1s1 (one electron with a 1s orbital wavefunction)

Ground state electron configuration for helium:

He = 1s2 (two electrons with 1s orbital wavefunctions)

Quantum numbers for each He e-:n = 1, l = 0, ml = 0, ms = +½n = 1, l = 0, ml = 0, ms = -½

Page 15: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ELECTRONS ON ATOMSHydrogen Electron Helium Electrons

Ener

gy (J

)

0

1s

2s

Ener

gy (J

)

0

1s

2s

Page 16: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ORDER OF FILLING SUBLEVELSElectrons occupy orbitals based on the Aufbau principle, they fill the

lowest subshells first and build up from there.

Page 17: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

MANY-ELECTON ATOM ENERGY DIAGRAM

Page 18: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUESTIONHow many electrons in an atom can be

in a 4p orbital?

Answer:A: 2B: 3C: 4D: 6E: 8

4p 4p 4p

Page 19: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUESTIONIn an atom, what is the maximum number of

electrons that can have the quantum numbers: n = 4 and ms = +½

Answer:A: 4B: 8C: 16D: 32E: 64

Page 20: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

LECTURE OBJECTIVES• Chapter 6.3

• Use quantum numbers to express specific electronic orbitals.

• Apply appropriate rules to the filling of electrons in atomic orbitals.

• Chapter 6.4

• Derive the predicted ground-state electron configurations of atoms

• Identify and explain exceptions to predicted electron configurations for atoms and ions

• Relate electron configurations to element classifications in the periodic table

• Chapter 6.5

• Describe and explain the observed trends in atomic size, ionization energy, and electron affinity of the elements

Page 21: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUESTIONWhat is the ground state electronic

configuration of lithium (Z = 3)?

2p3

2s22p1

1s22p1

1s22s1

1s3

Answer:ABCDE

Page 22: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

GROUND STATE CONFIGURATION OF LITHIUM

• Lithium (three electrons):

• Pauli exclusion principle prevents all three electrons from being in the 1s level (Li ≠ 1s3)

• So where does the third electron go; 2s or 2p level?

• The 2s orbital is able to penetrate closer to the nucleus, making it more stable and favored by the electron.

Page 23: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

THE EFFECT OF L ON ENERGY

Page 24: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ENERGY STATES OF ATOMS• Ground State

• Lowest energy arrangement of electrons in an atom: Li = 1s22s1

• Excited State

• Any allowed electron configuration that is not the ground state: Li = 1s22p1

• Forbidden State

• Impossible electron configurations (Pauli): Li = 1s3

Hund’s Rule:Lowest energy state occurs when there are the greatest number of

unpaired electrons with parallel spins.

Page 25: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ORBITAL FILLING

Pairing of electrons only occurs when all sublevels of the orbital have an electron.

Page 26: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

WRITING ELECTRON CONFIGURATIONS

1s22s1

1s22s2

1s22s22p1

1s22s22p2

1s22s22p3

1s22s22p4

1s22s22p5

1s22s22p6

Li =Be =B =C =N =O =F =

Ne =

FullLi =

Be =B =C =N =O =F =

Ne =

[He]2s1

[He]2s2

[He]2s22p1

[He]2s22p2

[He]2s22p3

[He]2s22p4

[He]2s22p5

[He]2s22p6

Condensed

Page 27: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

CLASSIFYING ELECTRONS IN AN ATOM

• Valence Electrons

• Electrons in the highest energy level of the atom are valence electrons - electrons with the largest value for n.

• Valence electrons are the ones that are chemically important.

• Core Electrons

• Electrons in the filled lower energy levels of the atom.

Page 28: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ELECTRON CONFIGURATIONS FOR GROUPS

Group 2Be =Mg =Ca =Sr =Ba =

[He]2s2

[Ne]3s2

[Ar]4s2

[Kr]5s2

[Xe]6s2

2 valance electrons

[He]2s22p5

[Ne]3s23p5

[Ar]3d104s24p5

[Kr]4d105s25p5

F =Cl =Br =

I =

Group 7

7 valance electrons

Page 29: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

TRANSITION METALS

• The transition metals have electrons in the d orbitals.

• There are a pair of exceptions to the normal electron filling in the transition metals (Cr and Cu).

• These exceptions occur because they are lower in energy than the normal electron filling pattern.

• The exception continues down those groups (Cr, Mo, W & Cu, Ag, Au).

Page 30: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

WHAT AFFECTS ATOMIC ORBITAL ENERGIES?

• The Nuclear Charge (Zeffective)

• Higher nuclear charge lowers orbital energy (stabilizes the system) by increasing the nucleus-electron attractions.

• Electron Repulsions (Shielding)

• Additional electrons in the same orbital raise orbital energy through electron-electron repulsions.

• Additional electrons in inner orbitals shield outer electrons more effectively than do electrons in the same sublevel.

Page 31: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

EFFECTIVE NUCLEAR CHARGE (ZEFF)

• The nuclear charge “experienced” by an electron in a many-electron atom is not the same as the actual charge of the nucleus.

• Zeff is specific for each electron in the atom.

• Zeff is always less than the full nuclear charge (Z) of the atom, due to electron shielding.

• For a 1s electron in a helium atom (Z=2), Zeff = +1.69

Page 32: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUESTIONFor which of these one-electron species is it

most difficult to remove the electron?

He+

Li2+

Be3+

B4+

Don’t know

Answer:ABCDE

Page 33: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ATOMIC PROPERTIES• Group Trends

• Variations in atoms of the same group are principally due to differences in the principal quantum number (n) for the valence electrons. (e.g. O, S, Se, Te, Po)

• Periodic Trends

• Variations in atoms along a period are principally due to the differences in the Zeff of the nucleus (e.g. B, C, N, O, F)

Page 34: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ATOMIC RADII• Atoms are, as you would expect, very small. The size of atoms is

typically measured in picometers (pm): 1 pm = 1×10-12 m or in Ångstroms (Å): 1Å = 1×10-10 m; 1Å = 100 pm

• The atomic radius is the sphere around the nucleus limited to the distances which the electrons can reach.

• The radius of an atom is not a fixed quantity; it will vary depending on the environment of the atom.

• The atomic radius is determined through measurements of the internuclear distances of molecules and compounds.

Page 35: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

METALLIC RADII

• Defined as half the shortest distance between nuclei of adjacent atoms in a crystal of the element.

• Aluminum:

• Internuclear distance: 286 pm

• Atomic radius: 143 pm

Page 36: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

COVALENT RADII• Two ways of determining the

covalent radius of an atom:

• Measured as half the bond length for the diatomic molecule (e.g. O2).

• By measuring the bond length between two atoms (e.g. CO) when the covalent radius of one of the atoms is known (e.g. O).

Page 37: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

MAIN-GROUP ATOMIC RADII

The atomic radii of the main-group elements increase down each group and from left to right across a period.

Transition elements are less systematic.

Page 38: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

PERIODICITY OF ATOMIC RADII

Page 39: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUESTIONWhich sequence of atoms is listed in

the correctly in order of increasing size?

F < Br < Ge < KNa < Al < P < S

Ba < Ca <Mg < BeCl < Si < C < B

Answer:ABCD

Page 40: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

IONIZATION ENERGY (IE)• The ionization energy is the energy needed to remove

an electron from a gas phase atom or ion.

• A(g) → A+(g) + e-(g) ∆E = IE1 for A

• A+(g) → A2+(g) + e-(g) ∆E = IE2

• The ionization energies are always positive and always increase for each subsequent electron to be removed.

• IE1 < IE2 < IE3 < ...

Page 41: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

IONIZATION ENERGIES

• Beryllium (1s22s2) ionization energies increase as follows:

• IE1 = + 900 kJ/mol (1s22s1)

• IE2 = + 1,760 kJ/mol (1s2)

• IE3 = + 14,850 kJ/mol (1s1)

• Removal of core electrons requires much more energy.

Page 42: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

IONIZATION ENERGY TREND

Page 43: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

IONIZATION ENERGY (IE)Which element has the greatest first

ionization energy (IE1)?

Li - [He]2s1

Na - [Ne]3s1

C - [He]2s22p2

O - [He]2s22p4

520 kJ/mol

496 kJ/mol

1086 kJ/mol

1314 kJ/mol

152 pm

186 pm

77 pm

73 pm

Page 44: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

PERIODICITY OF IONIZATION ENERGIES (IE1)

Page 45: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

First ionization energies of the main-group elements.

Generally increase up the groups and increase from left to right across a period.

Page 46: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

QUESTIONList these atoms in order of increasing first

ionization energy: Li, Na, C, O, F

Li < Na < C < O < FNa < Li < C < O < FF < O < C < Li < NaNa < Li < C < F < O

Answer:ABCD

Page 47: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

ELECTRON AFFINITY (EA)

• The electron affinity is the energy change (∆E) associated with adding an electron to a gas phase atom or ion.

• A(g) + e-(g) → A-(g) ∆E = EA1 for A

• The electron affinities can be either positive or negative - depending on the specific element.

• Periodic trends for EA are not as obvious as IE or radius.

Page 48: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

Main-group electron affinities.

Page 49: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

IONIC RADII

• The ionic radius is a measure of the size of ions.

• The radius can vary dramatically based on the environment that the ion is found within.

• The ionic radius is determined through measurements of the internuclear distances of ionic compounds.

Page 50: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

IONIC RADII TRENDS• Cations are smaller than their parent atoms:

• Li = 152 pm Li+ = 76 pm

• Anions are larger than their parent atoms:

• F = 72 pm F- = 133 pm

• The ionic radii increase down a group

• Li+ = 76 pm Na+ = 102 pm

Page 51: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

PROBLEMWhich ion has the largest radius?

Ion Electrons Protons Radius

Ca2+ 18 20 100 pm

Cl- 18 17 181 pm

K+ 18 19 138 pm

S2- 18 16 184 pm

Page 52: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

IONIC RADII

Have valence electrons equivalent to Neon (ioselectronic ions)

Page 53: Lecture 21 & 22...Orbital shape magnetic m l Integers from -l to 0 to +l Orbital orientation spin m s +½ or - ½ Direction of e-spin Spin up = +½ ↑ Spin down = -½ ↓ Two e-per

MAIN-GROUP IONS & NOBLE GAS CONFIGURATIONS