2.3 Charge-Induced Dipole Interaction

Slides:



Advertisements
Similar presentations
Electric Fields in Matter
Advertisements

Various Polarization Processes
1 Physical Chemistry III Molecular Interactions Piti Treesukol Chemistry Department Faculty of Liberal Arts and Science Kasetsart University :
Chapter 21, Electric Charge, and electric Field. Charles Allison © Electric Charge, q or Q Charge comes in two types 1e = 1.6x Coulombs.
Chapter 4 Electrostatic Fields in Matter
Dielectrics.
Chapter 6 Dielectrics: I Electric Polarization P Bound Charges Gauss ’ Law, Electric Displacemant D.
 Lecture 3 .  Dielectric Materials  Dielectric materials are also called as insulators.  In dielectric materials, all the electrons are tightly bound.
Sinai University Faculty of Engineering Science Department of Basic sciences 5/20/ From Principles of Electronic Materials and Devices, Third Edition,
Dielectrics Physics 101F. Introduction and Molecular Theory Dielectric are the insulators which are highly resistant to the flow of an electric current.
CHAPTER 7: Dielectrics …
From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005) These PowerPoint color diagrams can only be used by.
Electric Charge, Force, and Field
Lecture 3111/18/05. Electron Pair Geometries Molecules with only single covalent bonds around central atom. Axial atomsEquatorial atoms.
U Electric Field Lines u Eletric Dipoles u Torque on dipole in an external field u Electric Flux u Gauss’ Law.
Chapter 21 & 22 Electric Charge Coulomb’s Law This force of repulsion or attraction due to the charge properties of objects is called an electrostatic.
ELECTRIC AND MAGNETIC FIELD INTERACTIONS WITH MATERIALS By: Engr. Hinesh Kumar (Lecturer)
1 Physical Chemistry III Molecular Interactions Piti Treesukol Chemistry Department Faculty of Liberal Arts and Science Kasetsart University :
New Way Chemistry for Hong Kong A-Level Book 11 Chapter 9 Intermediate Type of Bonding 9.1Incomplete Electron Transfer in Ionic Compounds Ionic Compounds.
1 2.2 Charge-Dipole Interaction Review (Isr2011, sec 4.1) What is a dipole? How are polar molecules formed? Order of magnitude of molecular dipole Charge-Dipole.
Copyright © 2009 Pearson Education, Inc. Lecture 4 – Electricity & Magnetism (Electrostatics) a. Electric Charge, Electric Field & Gauss’ Law.
Chapter 16 Electric Charge and Electric Field. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom.
Electric Charge and Electric Field
Capacitors Q D A capacitor is a device that is capable of storing electric charges and thus electric potential energy. => charging Its purpose is to release.
Intermolecular Forces:Electrostatics “Dielectrics Different classical electrostatic interactions.
1 Fall, 2013 Instructor: J.-W. John Cheng Mech. Engr. Dept., Nat ’ l Chung Cheng Univ. Ch 2. Intermolecular Energies Interfacial Physics and Thin-Film.
Chapter 24: Electric Potential 24-2: Electric potential energy Coulomb ’ s law looks like the gravitation law. Hence, it is conservative. What does it.
Molecular Geometry 6.5. Hybridization Mixing of two or more atomic orbitals of similar E’s on the same atom to produce new hybrid atomic orbitals of =
Copyright © 2009 Pearson Education, Inc. Molecular Description of Dielectrics.
Announcements  Homework for tomorrow… (Ch. 26, Probs. 22 & 50) CQ 8: 2nC/cm : a) 0b) –(4.1 x 10 3 N/C)ihat 26.42: Lim_{z KQz/R 3, Lim_{z>>R} ->
Intermolecular and Intramolecular Forces Review. In the compound PCl 3, how many valence electrons are present?
COVALENT BONDS, DRAWING AND NAMING MOLECULES, AND MOLECULAR SHAPES COVALENT COMPOUNDS.
1 ENE 325 Electromagnetic Fields and Waves Lecture 5 Conductor, Semiconductor, Dielectric and Boundary Conditions.
Chemical Bonding.
Electric Fields in Matter  Polarization  Electric displacement  Field of a polarized object  Linear dielectrics.
Intermolecular Interactions
-q+q s We can define a vector called the dipole moment ( 电矩 ). Magnitude: Direction: from the negative (-) charge to the positive (+) charge. NOTE: This.
Chemical Bonds & Molecular Attractions Chapter 12.
Section 12.1 Characteristics of Chemical Bonds 1.To understand why atoms form bonds 2.To learn about ionic and covalent bonds and explain how they are.
Chapter 16 Electric Charge and Electric Field. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom.
Last Time Electric forces are stronger than gravitational forces Electric field of: Superposition Principle E tot is the sum from all charges Point Charges.
Chemical Bonding And Molecular Geometry. What is a chemical bond? - mutual electrical attraction between the nuclei and valence electrons of different.
Chapter 15 Matter and Electric Fields. What is the direction of the electric field at location X, due to the dipole? Question 1 (Chap. 14) A C B E D -
Electric Charge and Electric Field
Molecular Description of Dielectrics
-Atomic View of Dielectrics -Electric Dipole in an Electric Field -Partially Filled Capacitors AP Physics C Mrs. Coyle.
Chapter 6 Dielectrics: I
Covalent Bonds, Drawing and Naming Molecules, and Molecular Shapes
Lecture 01: Electric Fields & Forces
Fields & Forces Coulomb’s law Q r q How does q “feel” effect of Q?
Ch4. (Electric Fields in Matter)
Physical Properties of Molecules
Intermolecular Forces
Types of Chemical Bonds Chapter 8
Molecular Geometry VSEPR Theory- “Valence- shell, electron-pair repulsion” states that repulsion between the sets of valence-level electrons surrounding.
Intermolecular Forces
Covalent Bonding Electron Sharing.
Covalent Bonding Electron Sharing.
Intermolecular Forces
A Model for the Electrical Nature of Matter
8-3 Intermolecular forces
Molecular Geometry VSEPR Theory- “Valence- shell, electron-pair repulsion” states that repulsion between the sets of valence-level electrons surrounding.
Chapter 6 Bonding.
Lecture 1: MATTER POLARIZATION AND RELATIVE PERMITTIVITY
to a positively charged glass rod
+ + - If it loses an electron the atom now has one too many protons in the nucleus. The atom now has a positive charge and is called an ION. This happens.
Phys102 Lecture 4 Electric Dipoles
Intermolecular Forces
Chapter 15 Matter and Electric Fields
Phys102 Lecture 4 &5 Electric Dipoles
Presentation transcript:

2.3 Charge-Induced Dipole Interaction What Is Induced Dipole? Polarizability of non-polar atoms or molecules Charge-Induced Dipole Interaction Free energy of charge-induced dipole interaction in medium Polarizability of polar atoms or molecules

What Is Induced Dipole? Consider a electrically neutral atom Where valence electrons are uniformly distributed around the nucleus Placed within an external electrical field Eext Due to attractive force on electron and repulsive force on nucleus by Eext, distribution of valence electrons are no longer uniform induced dipole electron cloud atom radius R nucleus Eext = 0 Eext

A Rough Estimate of Induced Dipole Viewing atom as a nucleus with a rotating electron at fixed orbit normal to E E causing the electron to shift by a distance l Resulting in an effective dipole el  uind By force balance we have R E  l

Polarizability of Non-Polar Molecules From above estimate, the induced dipole is proportional to E and has the same direction The proportional constant is called the polarizability 0 of the molecule Polarizability of Some Atoms & Molecules He: 0.2 in unit of (40)Å3 CH4: 2.6 ■ CO2: 4.0

Polarizability of Non-Polar Molecules contd Example Consider sodium ion Na+ situated 0.4 nm away from the center of a methane molecule CH4 Calculate the induced dipole on CH4 Ans: 0.78 D

Free Energy of Charge-Induced Dipole Interaction in Isolation Force F(r) on the molecule with induced dipole by the charge at distance r: Free energy w(r) between charge and induced dipole: =

Polarizability of Polar Molecules in Medium In an electrical field Eext, a polar molecule experiences two effects (1) orientation effect as discussed in charge-dipole interaction in medium (2) induced dipole effect due to separation of nucleus and electron cloud as discussed for non-polar molecules

Polarizability of Polar Molecules in Medium contd Alignment of molecular dipole u along Eext Without Eext, a molecular dipole in medium appears as a zero net dipole in average With Eext, the molecular dipole tends to align with Eext according to Boltzmann distribution: Free energy between Q and u = - uEcos … (following the same procedure as that in charge-dipole interaction) we have free energy between charge and the oriented dipole:

Polarizability of Polar Molecules in Medium contd Free energy between electrical field E and a polar molecule in medium becomes Logically, some calls the extra term “orientation polarizability orient” due to dipole alignment to E

Polarizability of Polar Molecules in Medium contd Total polarizability  of polar molecules Induced dipole of polar molecules by E