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Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: [email protected] Office: CTH 311 Phone 257-4941 Office Hours: M,W 8:00-9:00 & 11:00-12:00 am; Tu,Th, F 9:30 - 11:30 a.m. April 7 , 2015: Test 1 (Chapters 1, 2, 3) April 30, 2015: Test 2 (Chapters 5, 6 & 7) May 19, 2015: Test 3 (Chapters. 19 & 20) May 19, Make Up: Comprehensive covering all Chapters Chemistry 481(01) Spring 2015

Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: [email protected] Office: CTH 311 Phone 257-4941 Office Hours:

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Page 1: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-1Chemistry 481, Spring 2015, LA Tech

Instructor: Dr. Upali Siriwardane

e-mail: [email protected]

Office: CTH 311 Phone 257-4941

Office Hours:

M,W 8:00-9:00 & 11:00-12:00 am;

Tu,Th, F 9:30 - 11:30 a.m.

April 7 , 2015: Test 1 (Chapters 1,  2, 3)

April 30, 2015: Test 2 (Chapters  5, 6 & 7)

May 19, 2015: Test 3 (Chapters. 19 & 20)

May 19, Make Up: Comprehensive covering all Chapters

Chemistry 481(01) Spring 2015

Page 2: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-2Chemistry 481, Spring 2015, LA Tech

Origin of Elements in the Universe Scientists have long based the origin of our Universe on the Big Bang Theory. According to

this theory, our universe was simply an expanding fairly cold entity consisting of only Hydrogen

and Helium during it's incipient stages. Over the expanse of many years, and through a

continuing process of fusion and fission, our universe has come to consist of numerous chemical

elements, four terrestrial planets(Earth, Mars, Venus, and Mercury), and five giant gas

planets(Saturn, Jupiter, Neptune, Pluto, and Uranus).

Page 3: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-3Chemistry 481, Spring 2015, LA Tech

Predicted Nuclear Fusion ofLight Elements in the Young,Hot Universe

Page 4: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-4Chemistry 481, Spring 2015, LA Tech

Few minutes after big Bang

Page 5: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-5Chemistry 481, Spring 2015, LA Tech

Eight Steps in the History of the Earth

1. The Big Bang

2. Star Formation

3. Supernova Explosion

4. Solar Nebula Condenses

5. Sun & Planetary Rings Form

6. Earth Forms

7. Earth's Core Forms 

8. Oceans & Atmosphere Forms

Page 6: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-6Chemistry 481, Spring 2015, LA Tech

Nuclear Burning

Page 7: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-7Chemistry 481, Spring 2015, LA Tech

Origin of the Elements: Nucleosynthesis

•Elements formed in the universe's original stars

were made from hydrogen gas condensing due to gravity. These young stars "burned" hydrogen in fusion reactions to produce helium and the hydrogen was depleted. Reactions such as those below built up all the heavier elements up to atomic number 26 in the periodic table.•When the stars got old they exploded in a super

nova, spreading the new elements into space with high flux of neutrons to produce heavy elements by neutron capture.

Page 8: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-8Chemistry 481, Spring 2015, LA Tech

1. What are the two basic types of nuclear reactions? Give examples of each that occur during the formation of the Universe

Page 9: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-9Chemistry 481, Spring 2015, LA Tech

Cosmic Abundances

Page 10: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-10Chemistry 481, Spring 2015, LA Tech

Balancing Nuclear ReactionsTwo conditions must be met to balance nuclear reactions:

1. The sum of the masses of the reactants must equal the sum of the masses of the products. (i.e., the values of A must balance on both sides of the equation.)

2. The sum of the protons for the reactants must equal the sum of the protons for the products. (i.e., the values of Z must balance on both sides of the equation.)

Page 11: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-11Chemistry 481, Spring 2015, LA Tech

Balancing Nuclear Reactions2. Complete the following Nuclear reactions:

a) Uranium – 238 decays by alpha radiation to produce what other element?

b) Uranium – 238 decays by alpha radiation to produce what other element?

c) What element did we start out with if the result of beta decay is bismuth– 214?

Page 12: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-12Chemistry 481, Spring 2015, LA Tech

Balancing Nuclear Reactions2. Complete the following Nuclear reactions:

d) What element is produced when mercury – 201 captures an inner shell electron with the production of a gamma ray to release excess energy?

Page 13: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-13Chemistry 481, Spring 2015, LA Tech

3. Predict the most likely modes of decay and the products of decay of the following nuclides:17F:

 

105Ag:    

 185Ta:

Page 14: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-14Chemistry 481, Spring 2015, LA Tech

Bonding Energy Curve

Page 15: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-15Chemistry 481, Spring 2015, LA Tech

Nuclear Binding EnergyThe binding energy of a nucleus is a measure of how

tightly its protons and neutrons are held

together by the nuclear forces. The binding energy per nucleon, the energy required to remove

one neutron or proton from a nucleus, is a function of the mass number A. (Dm) –mass defect

(Dm) = Mass of Nuclide - mass of (p + n +e )

Proton mass: 1.00728 amu

Neutron mass: 1.00867 amu

Electron mass: 0.00055 amu

Massdefect (Dm), then multiply by 931.5 MeV/amu

Page 16: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-16Chemistry 481, Spring 2015, LA Tech

4. Using the binding energy calculator, calculate the binding energy 235U if the mass of the this nuclide (isotope) is 235.0349 amu. ( P= 1.007277 amu, N= 1.008665 amu, e- =0.0005438 amu )

Page 17: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-17Chemistry 481, Spring 2015, LA Tech

5. What are theories that have been used to describe the nuclear stability?

Page 18: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-18Chemistry 481, Spring 2015, LA Tech

Stability of the Elements and Their Isotopes

P/N Ratio

Why are elements

With Z > 82 are

Unstable?

Page 19: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-19Chemistry 481, Spring 2015, LA Tech

Magic Numbers• Nuclei with either numbers of protons or

neutrons equal to Z, N =2 (He), 8(O), 20 (Ca), 28(Si), 50(Sn, 82(Pb), or 126(?)(I)

• exhibit certain properties which are analogous to closed shell properties in atoms, including

• anomalously low masses, high natural abundances and high energy first excited states.

Page 20: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-20Chemistry 481, Spring 2015, LA Tech

The Kinetics of Radioactive DecayNuclear reactions follow 1st order kinetics

Page 21: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-21Chemistry 481, Spring 2015, LA Tech

6. How long would it take for a sample of 222Rn that weighs 0.750 g to decay to 0.100 g?  Assume a half-life for 222Rn of 3.823 days?

Page 22: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-22Chemistry 481, Spring 2015, LA Tech

7. The skin, bones and clothing of an adult female mummy discovered in Chimney Cave, Lake Winnemucca, Nevada, were dated by radiocarbon analysis.  How old is this mummy if the sample retains 73.9% of the activity of living tissue?

Page 23: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-23Chemistry 481, Spring 2015, LA Tech

Bohr model of the atom

Balmer later determined an empirical relationship that described the spectral lines for hydrogen.

DE = - 2.178 x 10-18

m-1 =

( )1

nf2

1

ni2-

nf = 2 ni = 3,4, 5, . . . Blamer series

Spectra of many other atoms can be described by

similar relationships.

Page 24: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-24Chemistry 481, Spring 2015, LA Tech

Bohr model of the atom

• The Bohr model is a ‘planetary’ type model.

• Each principal quantum represents a new ‘orbit’ or layer.

• The nucleus is at the center of the model.

• RH = 2.178 x 10-18 JEn = -

En = RH

Page 25: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-25Chemistry 481, Spring 2015, LA Tech

Emission Spectrum of Hydrogen•

Bohr studied the spectra produced when atoms were excited in a gas discharge tube.

He observed that each element produced its

own set of characteristic lines.

Page 26: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-26Chemistry 481, Spring 2015, LA Tech

Emission Spectrum of Hydrogen

• Line Spectrum• Energy is absorbed when an electron goes from a

lower(n) to a higher(n) • Energy is emitted when an electron goes from a

higher(n) to a lower(n) level

• Energy changed is given by:DE = Ef - Ei

• or DE = -2.178 x 10-18 [1/n2f - 1/n2

i] J

• DE is negative for an emission and positive for an absorption

• DE can be converted to l or 1/ l by l = hc/E.

Page 27: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-27Chemistry 481, Spring 2015, LA Tech

What is Bohr’s Atomic model?

• explain emission spectrum of hydrogen atom• applied the idea of Quantization to electrons to orbits• energies of these orbits increase with the distance

from nucleus.

• Energy of the electron in orbit n (En):

• En = -2.178 x 10-18 J (Z2/n2)

• En = -2.178 x 10-18 J 1/n2; Z=1 for H

Page 28: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-28Chemistry 481, Spring 2015, LA Tech

Bohr model of the atom

Balmer later determined an empirical relationship that described the spectral lines for hydrogen.

DE = - 2.178 x 10-18

J ( )1

nf2

1

ni2-

nf = 2 ni = 3,4, 5, . . . Blamer series

Spectra of many other atoms can be described by

similar relationships.

En = -

Page 29: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-29Chemistry 481, Spring 2015, LA Tech

Paschen, Blamer and Lyman Series

Page 30: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-30Chemistry 481, Spring 2015, LA Tech

Calculation using the equation: E = -2.178 x 10-18 (1/nf

2 - 1/ni2 ) J, Calculate

the wavelength of light that can excite the electron in a ground state hydrogen atom to n = 7 energy level.

Page 31: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-31Chemistry 481, Spring 2015, LA Tech

The energy for the transition from n = 1 to n = 7:

DE = -2.178 x 10-18 J [1/n2f - 1/n2

i]; nf = 7, ni = 1

DE = -2.178 x 10-18 [1/72 - 1/12] J

DE = -2.178 x 10-18 [1/49 - 1/1] J

DE = -2.178 x 10-18 [0.02041 - 1] J

DE = -2.178 x 10-18 [-0.97959] J

= 2.134 x 10-18 J (+, absorption)

calculate the l using l = hc/E 6.626 x 10-34 Js x 3.00 x 108 m/s

l = ---------------------- 2.13 x 10-18 J l = 9.31 x 10-8 m

Calculation using Bohr eqaution

Page 32: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-32Chemistry 481, Spring 2015, LA Tech

8. Using Bohr energy calculator, calculate the wavelength of light that can excite the electron in a ground state hydrogen atom from n = 5 to n = 3 energy level.

Page 33: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-33Chemistry 481, Spring 2015, LA Tech

Wave theory of the electron• 1924: De Broglie suggested that electrons

have wave properties to account for why their energy was quantized.

• He reasoned that the electron in the hydrogen atom was fixed in the space around the nucleus.

• He felt that the electron would best be represented as a standing wave.

• As a standing wave, each electron’s path must equal a whole number times the wavelength.

Page 34: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-34Chemistry 481, Spring 2015, LA Tech

De Broglie proposed that all particles have a wavelength as related by:

l = wavelength, meters

h = Plank’s constant

m = mass, kg

v = frequency, m/s

De Broglie waves

l =h

mv

Page 35: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-35Chemistry 481, Spring 2015, LA Tech

Constructively Interfered 2D-Wave

Page 36: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-36Chemistry 481, Spring 2015, LA Tech

destructively Interfered 2D-Wave

Page 37: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-37Chemistry 481, Spring 2015, LA Tech

Two-dimensional wave - Vibrations on a Drumskin One circular node

(at the drumskin's edge)

Two circular nodes

(one at the drumskin's edge plus

one more)

Three circular nodes

(one at the drumskin's edge plus

two more)

One transverse node

(plus a circular one at the

drumskin's edge)

Two transverse nodes

(plus one at the drumskin's

edge)

Page 38: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-38Chemistry 481, Spring 2015, LA Tech

What is a wave-mechanical model?• motions of a vibrating string shows one dimensional motion.• Energy of the vibrating string is quantized• Energy of the waves increased with the nodes. • Nodes are places were string is stationary. • Number of nodes gives the quantum number. One

dimensional motion gives one quantum number.

Vibrating String : y = sin(npx/l)

d2y/dx2 = -(n2p2/l2)sin(npx/l) = -(n2p2/l2)y

Page 39: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-39Chemistry 481, Spring 2015, LA Tech

Quantum model of the atom• Schrödinger developed an equation to

describe the behavior and energies of electrons in atoms.

• His equation ( Wave function ) is similar to one used to describe electromagnetic waves. Each electron can be described in terms of Wave function its quantum numbers. n, l, ml, ms),

• 2 is proportional probablity of finding the electron in a given volume. Max Born Interpretation: 2 = atomic orbital

Page 40: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-40Chemistry 481, Spring 2015, LA Tech

Schrödinger Equation

= wave function

E = total energy

V = potential energy

Page 41: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-41Chemistry 481, Spring 2015, LA Tech

Schrödinger Equation

= wave function E = total energy V = potential energy

Page 42: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-42Chemistry 481, Spring 2015, LA Tech

Schrödinger Equation in Polar Coordinates

Page 43: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-43Chemistry 481, Spring 2015, LA Tech

Polar Coordinates

Page 44: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-44Chemistry 481, Spring 2015, LA Tech

Quantum Model of atom• Electrons travel in three dimensions• Four quantum numbers are needed• three to describe, x, y, z, and four for the spin• four quantum numbers

describe an orbital currently used to explain the arrangement, bonding and spectra of atoms.

Page 45: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-45Chemistry 481, Spring 2015, LA Tech

Four Quantum Numbers of the Atom• n value could be

1, 2, 3, 4, 5, 6. 7. . . etc.• l values depend on n value: can have

0 . . . (n - 1) values

• ml values depends on l value:

can have -l . , 0 . . . +l values of ml

• ms values

should always be -1/2 or +1/2

Page 46: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-46Chemistry 481, Spring 2015, LA Tech

Solutions to Shrődinger Equation

Series of allowed discrete values:

n, l, ml, ms

n = 1,2,3,4,5,6,7..etc.

En = -

Page 47: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-47Chemistry 481, Spring 2015, LA Tech

Components of Mathematical expression of hydrogen like orbitals

in polar coordinates:

n, l, ml, ms (r,,) = R n, l, (r) Y l, ml, (,)

R n, l, (r ) = Radial Wave Function

Y l, ml, (,) =Angular Wave Function

[R n, l (r )]2 or 4pr2R2 = Radial Distribution Function or Pnl(r).

Page 48: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-48Chemistry 481, Spring 2015, LA Tech

Radial Distribution Function, Pnl(r).This is defined as the probability that an electron in

the orbital with quantum numbers n and l will be found at a distance r from the nucleus. It is related to the radial wave function by the following relationship:

                      ; normalized by                

Page 49: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-49Chemistry 481, Spring 2015, LA Tech

9. Describe the Schrödinger equation and the breaking up of wave function, into radial and

angular component of a wave function and explain the general rule used to find the number

of radial and angular nodes of a wave function.

Page 50: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-50Chemistry 481, Spring 2015, LA Tech

s orbitals

R n, l, (r) only no Y l, ml, (,)

s-Atomic Orbitals

Page 51: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-51Chemistry 481, Spring 2015, LA Tech

2s orbital

2s-Atomic Orbital: Probability distribution ψ2 for the 2s orbital

Page 52: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-52Chemistry 481, Spring 2015, LA Tech

2s

3s

s-Atomic orbitals

Page 53: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-53Chemistry 481, Spring 2015, LA Tech

p-Atomic orbitals

2p

3p

Page 54: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-54Chemistry 481, Spring 2015, LA Tech

Nodes in the Total nodes = n -1

Angular nodes = l

Radial nodes = n -1- l

Eg 4d orbital:

Total nodes = 4 -1 = 3

Angular nodes = l = 2

Radial nodes = n -1- l = 4-1-2 = 1

Page 55: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-55Chemistry 481, Spring 2015, LA Tech

10. Consider the following radial probability density-distribution plot and respond to the associated questions.

a) How many radial nodes are there?

b) If the total number of nodes is 3, what type of orbital is involved?

c) Which orbital would it be if there were one more node?

Page 56: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-56Chemistry 481, Spring 2015, LA Tech

.

Rnl(r) Pnl(r) n l

1s

                                                                              

        

1s

                                                    

                                  

1 0

2s

                                                                        

              

2s

                                                    

                                  

2 0

2p

                                                                                     

 

2p

                                                    

                                  

2 1

3s                                                                                       

3s

                                                    

                                  

3 0

3p                                                                                       

3p

                                                    

                                  

3 1

3d                                                                                       

3d

                                                    

                                  

3 2

Radial wavefunctions, Rnl(r), and the radial distribution functions, Pnl(r)

Page 57: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-57Chemistry 481, Spring 2015, LA Tech

d-orbitals(dxy, dxz, dyz, dz

2 , and dx

2-y

2

orbitals)

Page 58: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-58Chemistry 481, Spring 2015, LA Tech

f-orbitals( 4fy3 , 4fx3 , 4fz3 , 4fxz2y2 , 4fyz2x2 , 4fzx2y2 , and 4fxyz orbitals)

Page 59: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-59Chemistry 481, Spring 2015, LA Tech

Screening (shielding) constant (σ)Screening (shielding) constant (σ) for each electron is calculated based on:

the principle quantum number

orbital type and penetration and of all

other electrons in an atom.

σ gives Zeff .

Zeff = Z - σ; Z is the atomic number.

Page 60: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-60Chemistry 481, Spring 2015, LA Tech

Effective nuclear charge (Zeff)

Zeff is the nuclear charge felt by an electron in a multielectron atom:

a) Each electron in an atom has different Zeff.

b) Each Zeff is less than atomic number (Z) since electrons screen each other from the nucleus.

c) Zeff depends on the n and l quantum number of an electron.

d) Zeff Depends on orbital type the electron is in: Zeff of 4s > 4p > 4d > 4f.

Page 61: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-61Chemistry 481, Spring 2015, LA Tech

Radial Wave Funtions

Page 62: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-62Chemistry 481, Spring 2015, LA Tech

Radial Distribution Functions, Penetration and Shielding

Page 63: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-63Chemistry 481, Spring 2015, LA Tech

Penetration & Shielding of an Electron in Multi-electron Atom

Penetration of an electron:• Greater the penetration there is more chance of

electrons being located close to the nucleus.• Comparing s, p, d, or f orbitals within same shell (or

principle QN), penetration of an electrons are in the order: s > p > d > f

Shielding power of an electron:• Shields of other electrons depends penetration and the

orbital type. Shielding power of electrons in orbitals of that same shell are: s > p > d > f

Page 64: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-64Chemistry 481, Spring 2015, LA Tech

Slater Calculation of (Zeff)

Page 65: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-65Chemistry 481, Spring 2015, LA Tech

Slater Calculation of (Zeff)

Page 66: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-66Chemistry 481, Spring 2015, LA Tech

11. Cu: (1s2)(2s2, 2p6) (3s2,3p6) (3d10) (4s1) : there are two possible scenarios for forming Cu+ ion- ionizing 3d10 electron or 4s1. Using Slater’s Rules show which one of the electrons 4s or 3d would come out easily.If the electron is in a d or f-orbital:

All electrons in groups higher than the electron in question contribute zero to s.

  Each electron in the same group contributes 0.35 to s.

  All those in groups to the left contribute 1.0 to s (n-3) (n-2) (n-1) (n-1)

Cu: (1s2)(2s2, 2p6) (3s2,3p6) (3d10) (4s1)

s (4s1) = ( 10x1 ) ( 8x 0.85)(1X10) = 26.8 Zeff = 29 – 26.6 = 2.4

Cu: (1s2)(2s2, 2p6) (3s2,3p6) (3d10) (4s1)

s (3d1) = ( 18x1 ) ( 9x 0.35) (0) = 21.15 Zeff = 29 – 21.15 = 7.85

Page 67: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-67Chemistry 481, Spring 2015, LA Tech

Effective nuclear charge (Zeff) of Atomic Orbitals vs. Z (atomic number)

En = -

Page 68: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-68Chemistry 481, Spring 2015, LA Tech

How do you get the electronic configuration of an atom?

• Use periodic table• Periodic table is divided into orbital blocks• Each period:• represents a shell or n • Start writing electron configuration• Using following order1s 2s 2p 3s 3p 4s 3d 4p 5s 4d 5p 6s 4f 5d 6p 7s 5f 6d…

(building up (Auf Bau) principle:)

Page 69: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-69Chemistry 481, Spring 2015, LA Tech

ELECTRONIC CONFIGURATION OF MANY-ELECTRON ATOMS

• AUFBAU (GER. BUILDING UP) PRINCIPLE

• PAULI EXCLUSION PRINCIPLE• HUND’S RULE

Page 70: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-70Chemistry 481, Spring 2015, LA Tech

Tl

5d10

6s2

6p1

Hg

4f14

5d10

6s2

Au

4f14

5d10

6s1

Hf

4f14

5d2

6s2

Lu

4f14

5d1

6s2

Li

2s1

Na

3s1

Cs

6s1

Rb

5s1

K

4s1

Fr

7s1

Pt

4f14

5d9

6s1

Ir

4f14

5d7

6s2

Os

4f14

5d6

6s2

Re

4f14

5d5

6s2

W

4f14

5d4

6s2

Ta

4f14

5d3

6s2

H

1s1

He

1s2

Rn

5d10

6s2

6p6

At

5d10

6s2

6p5

Po

5d10

6s2

6p4

Bi

5d10

6s2

6p3

Pb

5d10

6s2

6p2

Cd

4d10

5s2

Ag

4d10

5s1

Zr

4d2

5s2

Y

4d1

5s2

Pd

4d10

Rh

4d8

5s1

Ru

4d7

5s1

Tc

4d5

5s2

Mo

4d5

5s1

Nb

4d3

5s2

Lr

6d1

7s2

Ba

6s2

Be

2s2

Mg

3s2

Sr

5s2

Ca

4s2

Ra

7s2

Zn

3d10

4s2

Cu

3d10

4s1

Ti

3d2

4s2

Sc

3d1

4s2

Ni

3d8

4s2

Co

3d7

4s2

Fe

3d6

4s2

Mn

3d5

4s2

Cr

3d5

4s1

V

3d3

4s2 In

4d10

5s2

5p1

Xe

4d10

5s2

5p6

I

4d10

5s2

5p5

Te

4d10

5s2

5p4

Sb

4d10

5s2

5p3

Sn

4d10

5s2

5p2

Ga

3d10

4s2

4p1

Kr

3d10

4s2

4p6

Br

3d10

4s2

4p5

Se

3d10

4s2

4p4

As

3d10

4s2

4p3

Ge

3d10

4s2

4p2

Al

3s2

3p1

Ar

3s2

3p6

Cl

3s2

3p5

S

3s2

3p4

P

3s2

3p3

Si

3s2

3p2

B

2s2

2p1

Ne

2s2

2p6

F

2s2

2p5

O

2s2

2p4

N

2s2

2p3

C

2s2

2p2

Gd

4f7

5d1

6s2

Cm

5f7

6d1

7s2

Tb

4f9

6s2Bk

5f9

7s2

Sm

4f6

6s2Pu

5f6

7s2

Eu

4f7

6s2Am

5f7

7s2

Nd

4f4

6s2

U

5f3

6d1

7s2

Pm

4f5

6s2

Np

5f4

6d1

7s2

Ce

4f1

5d1

6s2

Th

6f2

7s2

Pr

4f3

6s2

Pa

5f2

6d1

7s2

Yb

4f14

6s2No

5f14

7s2

La

5d1

6s2Ac

6d1

7s2

Er

4f12

6s2Fm

5f12

7s2

Tm

4f13

6s2Md

5f13

7s2

Dy

4f10

6s2Cf

5f10

7s2

Ho

4f11

6s2Es

5f11

7s2

Electronic Confn

Page 71: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-71Chemistry 481, Spring 2015, LA Tech

Using the periodic table• To write the ground-state electron configuration of

an element:

• Starting with hydrogen, go through the elements in order of increasing atomic number

• As you move across a period

• Add electrons to the ns orbital as you pass through groups IA (1) and IIA (2).

• Add electrons to the np orbital as you pass through Groups IIIA (13) to 0 (18).

• Add electrons to (n-1) d orbitals as you pass through IIIB (3) to IIB(12) and add electrons to (n-2) f orbitals as you pass through the f -block.

Page 72: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-72Chemistry 481, Spring 2015, LA Tech

Writing electron configurations

• Electron configurations can also be written for ions.

• Start with the ground-state configuration for the atom.

• For cations, remove a number of the outermost electrons equal to the charge.

• For anions, add a number of outermost electrons equal to the charge.

Page 73: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-73Chemistry 481, Spring 2015, LA Tech

Exception to Building Up Principle

a) Electronic Configuration of d-block and f-block elements

d5 or d10 and f7 or f14 are stable Cr :[Ar] 3d4 4s2 wrong

Cr :[Ar] 3d5 4s1 correct

Cu :[Ar] 3d9 4s2 wrong

Cu :[Ar] 3d10 4s1 correct

Page 74: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-74Chemistry 481, Spring 2015, LA Tech

Lanthanoids

Gd

4f7

5d1

6s2

Tb

4f9

6s2

Sm

4f6

6s2

Eu

4f7

6s2

Nd

4f4

6s2

Pm

4f5

6s2

Ce

4f1

5d1

6s2

Pr

4f3

6s2

Yb

4f14

6s2

La

5d1

6s2

Er

4f12

6s2

Tm

4f13

6s2

Dy

4f10

6s2

Ho

4f11

6s2

Page 75: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-75Chemistry 481, Spring 2015, LA Tech

Actinoids

Cm

5f7

6d1

7s2

Bk

5f9

7s2

Pu

5f6

7s2

Am

5f7

7s2

U

5f3

6d1

7s2

Np

5f4

6d1

7s2

Th

6f2

7s2

Pa

5f2

6d1

7s2

No

5f14

7s2

Ac

6d1

7s2

Fm

5f12

7s2

Md

5f13

7s2

Cf

5f10

7s2

Es

5f11

7s2

Page 76: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-76Chemistry 481, Spring 2015, LA Tech

Electronic Configuration of Transition Metal cations

d-block and f-block elements

d orbitals are lower in energy than s orbitals

f orbitals are lower in energy than d orbitals

E.g. Neutral atom Fe :[Ar] 3d6

4s2

Cation, Fe3+

:[Ar] 3d5

Exception to Building Up Principle

Page 77: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-77Chemistry 481, Spring 2015, LA Tech

12. Give the ground state electronic configurations of following in core format.

a) Mo

b) Ag

c) V3+

d) Mn2+

e) Cr2+

f) Co3+

g) Cr6+

h) Gd3+

Page 78: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-78Chemistry 481, Spring 2015, LA Tech

Magnetic Properties of Atoms a) Paramagnetism? attracted to magnetic field due to un-paired

electrons.

b) Ferromagnetism? attracted very strongly to magnetic field due to

un-paired electrons. c) Diamagnetism? Repelled by a magnetic field due to paired

electrons.

Page 79: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-79Chemistry 481, Spring 2015, LA Tech

13. Give the ground state electronic configurations of the following in valence orbital box format and give the number of unpaired electrons.

a) Mn:

b) Co:

c) Fe2+:

d) Nd3+:

Page 80: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-80Chemistry 481, Spring 2015, LA Tech

Periodic trends• Many trends in physical and chemical properties

can be explained by electron configuration.• We’ll look at some of the more important

examples.

Atomic radii

Ionic radii

First ionization energies

Electron affinities

Page 81: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-81Chemistry 481, Spring 2015, LA Tech

•Cations have smaller radii than neutral atoms.

•Anions have larger radii than neutral atoms

•The more charge on the ion more effect on the

radii.

How does Ionic radii of elements vary?

Page 82: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-82Chemistry 481, Spring 2015, LA Tech

14. How do you measure atomic (ionic) radii (size)?

Page 83: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-83Chemistry 481, Spring 2015, LA Tech

Atomic radii of elements going down a group?

Page 84: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-84Chemistry 481, Spring 2015, LA Tech

Lanthanoide Contration

• Filling of the 4f orbitals in the lanthanides, which occur within the third series of transition elements, causes these transition metals to be smaller than expected because the 4f orbitals are very poor nuclear shielders and Zeff of 6s2

obitals increase and the atomic radii decrease.• 3rd-series elements have nearly the same

effective nuclear charge as the 2nd-series elements, and thus, nearly the same size

Ce [Xe] 4f1

5d16s

2

Page 85: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-85Chemistry 481, Spring 2015, LA Tech

15. Why the atomic radius of Zr (1.64) which is in 5th period is almost similar to a element, Hf (1.65) in 6th period.

Page 86: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-86Chemistry 481, Spring 2015, LA Tech

Ionic radii

Cations

These are smaller than the atoms from which they are formed.

Anions

These are larger than the atoms from which there are formed..

Page 87: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-87Chemistry 481, Spring 2015, LA Tech

Isoelectronic configurations

Species that have the same electron configurations.

Example

Each of the following has an electron configuration of 1s2 2s2 2p6

O2- F- Ne

Na+ Mg2+ Al3+

Page 88: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-88Chemistry 481, Spring 2015, LA Tech

Ionization energy

• First ionization energy

The energy to remove one electron from a neutral atom in the gas phase.

• A(g) + first ionization energy A+(g) + e-

• This indicates how easy it is to form a cation.

Metals tend to have lower first ionization energies than nonmetals.

• They prefer to become cations.

Page 89: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-89Chemistry 481, Spring 2015, LA Tech

0

500

1000

1500

2000

2500

0 20 40 60 80 100

First ionization energyHe

Ne

Ar

Kr

Xe

Rn

Fir

st

ion

izati

on

en

erg

y (

kJ/

mol)

Atomic number

Page 90: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-90Chemistry 481, Spring 2015, LA Tech

Changes of I.E. Across a period

Page 91: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-91Chemistry 481, Spring 2015, LA Tech

16. Why is the ionization energy of P (11.00 eV) greater than S (10.36 eV)?

Page 92: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-92Chemistry 481, Spring 2015, LA Tech

•Electron Affinity depends on Zeff of the nucleus to the outermost electron in the

valence shell.

•Going down the group Zeff for the outer most shell decrease hence the Electron

Affinity also increase

•Going across the period Zeff for the outer most shell increase hence the Electron

Affinity also decrease

How does Electron Affinity vary in the periodic table?

Page 93: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-93Chemistry 481, Spring 2015, LA Tech

Electron affinity

Atomic number

Page 94: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-94Chemistry 481, Spring 2015, LA Tech

ElectronegativityThe ability of an atom that is bonded to another atom or

atoms to attract electrons to itself.

It is related to ionization energy and electron affinity.

It cannot be directly measured.

The values are unitless since they are relative to each other.

The values vary slightly from compound to compound but still provide useful qualitative predictions.

Page 95: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-95Chemistry 481, Spring 2015, LA Tech

Electronegativities

0.5

1

1.5

2

2.5

3

3.5

4

0 20 40 60 80 100

Ele

ctr

on

eg

ati

vit

y

Atomic number

Electronegativity is a

periodic property.

Electronegativity is a

periodic property.

Page 96: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-96Chemistry 481, Spring 2015, LA Tech

17. How you define electronegativity?

Page 97: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-97Chemistry 481, Spring 2015, LA Tech

Electronegativity Scales• Pauling Electronegativity, cP

• Mulliken Electronegativity, cM

• The Allred-Rochow, cAR

• Sanderson electronegativity

• Allen electronegativity

Page 98: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-98Chemistry 481, Spring 2015, LA Tech

Pauling Electronegativity, cP

EA-A and EB-B bond-energy of homonuclear A-A & B-B diatomic molecules

EA-B bond-energy of heteronuclear A-B diatomic molecule

cA cB are electronegativity values of A and B

Pauling comments that it is more accurate to use the geometric mean rather than the arithmetic mean

Page 99: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-99Chemistry 481, Spring 2015, LA Tech

Mulliken Electronegativity, cM

The Mulliken electronegativity can only be calculated for an element for which the electron affinity is known• For ionization energies and electron affinities in

electronvolts

• For energies in kilojoules per mole

Page 100: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-100Chemistry 481, Spring 2015, LA Tech

The Allred-Rochow, cAR

The effective nuclear charge, Zeff experienced by valence electrons can be estimated using Slater's rules, while the surface area of an atom in a molecule can be taken to be proportional to the square of the covalent radius, rcov. When rcov is expressed in ångströms,

Page 101: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-101Chemistry 481, Spring 2015, LA Tech

Sanderson, cs

Sanderson has also noted the relationship between electronegativity and atomic size, and has proposed a method of calculation based on the reciprocal of the atomic volume.

The simplest definition of electronegativity is that of Allen, bases on average energy of the valence electrons in a free atom

Allen, cA

where εs,p are the one-electron energies of s-

and p-electrons in the free atom and ns,p are

the number of s- and p-electrons in the valence

shell.

Page 102: Chapter-1-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-1-102Chemistry 481, Spring 2015, LA Tech

18. Calculate the electronegativity (X) (Xm, Xar)

for Cl. [ Xm= 1/2(I+Ae);

Xar= 0.744+ 0.359 Zeff/r2 ]

a) Xm When Ei and Eea kJ per mol

Xm= 1.97 x 10-3(1251 + 349 ) + 0.19

Xm = 3.342 (3.54)

a) Xar When r ( 0.99 Angstroms) and Zeff = 6.12

Xar= 0.359 Zeff/r2 + 0.744

Xar = 2.98 (2.83)