Preview chemical principles, 6th edition by peter atkins , loretta jones, leroy laverman (2013)

Preview Chemical Principles, 6th Edition by Peter Atkins , Loretta Jones, Leroy Laverman (2013) Preview Chemical Principles, 6th Edition by Peter Atkins , Loretta Jones, Leroy Laverman (2013) Preview Chemical Principles, 6th Edition by Peter Atkins , Loretta Jones, Leroy Laverman (2013) Preview Chemical Principles, 6th Edition by Peter Atkins , Loretta Jones, Leroy Laverman (2013) Preview Chemical Principles, 6th Edition by Peter Atkins , Loretta Jones, Leroy Laverman (2013)

CHEMICAL PRINCIPLES THE QUEST FOR INSIGHT Sixth Edition PETER ATKINS · LORETTA JONES · LEROY LAVERMAN FMTOC.indd Page i 10/18/12 8:07 PM user-F393 /Users/user-F393/Desktop SIXTH EDITION CHEMICAL PRINCIPLES THE QUEST FOR INSIGHT PETER ATKINS Oxford University LORETTA JONES University of Northern Colorado LEROY LAVERMAN University of California, Santa Barbara W H Freeman and Company New York FMTOC.indd Page ii 30/10/12 3:08 PM user-F408 /Users/user-F408/Desktop Associate Publisher: Jessica Fiorillo Library of Congress Control Number: Senior Developmental Editor: Randi Blatt Rossignol Your EPCN application for a Library of Congress control Marketing Manager: Alicia Brady Media and Supplements Editors: Dave Quinn and Heidi Bamatter Assistant Editor: Nicholas Ciani number for Title: “Chemical principles” ISBN: “1429288973” was successfully transmitted to the Library of Congress Photo Editor: Bianca Moscatelli Senior Project Editor: Georgia Lee Hadler ISBN-13: 978-1-4292-8897-2 Full-Service Project Management: Aptara ISBN-10: 1-4292-8897-3 Cover Designer: Victoria Tomaselli International Edition International Edition ISBN-13: 978-1-4641-2467-9 Cover design: Dirk Kaufman ISBN-10: 1-4641-2467-1 Cover image: Nastco/iStockphoto.com Text Designer: Marsha Cohen Illustration Coordinator: Bill Page Illustrations: Peter Atkins and Leroy Laverman with © 2013, 2010, 2005, 2002 by P W Atkins, L L Jones and L E Laverman All rights reserved Network Graphics Production Manager: Paul Rohloff Printed in the United States of America Composition: Aptara Printing and Binding: RR Donnelley First printing W H Freeman and Company 41 Madison Avenue New York, NY 10010 Houndmills, Basingstoke RG21 6XS, England www.whfreeman.com Macmillan Higher Education Houndmills, Basingstoke RG21 6XS, England www.macmillanhighered.com/international FMTOC.indd Page iii 10/18/12 8:07 PM user-F393 /Users/user-F393/Desktop Contents in Brief FUNDAMENTALS F1 Introduction and Orientation, Matter and Energy, Elements and Atoms, Compounds, The Nomenclature of Compounds, Moles and Molar Masses, Determination of Chemical Formulas, Mixtures and Solutions, Chemical Equations, Aqueous Solutions and Precipitation, Acids and Bases, Redox Reactions, Reaction Stoichiometry, Limiting Reactants Chapter THE QUANTUM WORLD Chapter QUANTUM MECHANICS IN ACTION: ATOMS 31 Chapter CHEMICAL BONDS 67 MAJOR TECHNIQUE • Infrared Spectroscopy 105 Chapter 107 MOLECULAR SHAPE AND STRUCTURE MAJOR TECHNIQUE • Ultraviolet and Visible Spectroscopy 146 Chapter THE PROPERTIES OF GASES 149 Chapter LIQUIDS AND SOLIDS 189 MAJOR TECHNIQUE • X-Ray Diffraction 223 Chapter INORGANIC MATERIALS 227 Chapter THERMODYNAMICS: THE FIRST LAW 259 Chapter THERMODYNAMICS: THE SECOND AND THIRD LAWS 317 Chapter 10 PHYSICAL EQUILIBRIA 367 MAJOR TECHNIQUE • Chromatography 419 Chapter 11 CHEMICAL EQUILIBRIA 421 Chapter 12 ACIDS AND BASES 463 Chapter 13 AQUEOUS EQUILIBRIA 519 Chapter 14 ELECTROCHEMISTRY 561 Chapter 15 CHEMICAL KINETICS 611 MAJOR TECHNIQUE • Computation 665 Chapter 16 THE ELEMENTS: THE MAIN-GROUP ELEMENTS 667 Chapter 17 THE ELEMENTS: THE d-BLOCK 725 Chapter 18 NUCLEAR CHEMISTRY 765 Chapter 19 ORGANIC CHEMISTRY I: THE HYDROCARBONS 797 MAJOR TECHNIQUE • Mass Spectrometry 821 Chapter 20 823 ORGANIC CHEMISTRY II: POLYMERS AND BIOLOGICAL COMPOUNDS MAJOR TECHNIQUE • Nuclear Magnetic Resonance 854 iii FMTOC.indd Page iv 10/18/12 8:07 PM user-F393 /Users/user-F393/Desktop Contents Preface FUNDAMENTALS Introduction and Orientation A B C D F1 F1 F2 F2 F4 F5 Matter and Energy F5 Physical Properties Force Energy Exercises F6 F10 F11 F15 Elements and Atoms F17 B.1 B.2 B.3 B.4 F17 F18 F20 F21 F24 Atoms The Nuclear Model Isotopes The Organization of the Elements Exercises Compounds F25 C.1 C.2 C.3 F25 F26 F27 F32 What Are Compounds? Molecules and Molecular Compounds Ions and Ionic Compounds Exercises The Nomenclature of Compounds D.1 D.2 D.3 Names of Cations Names of Anions Names of Ionic Compounds Exercises H I J K Names of Inorganic Molecular Compounds TOOLBOX D.2 • How to Name Simple Inorganic Molecular Compounds D.5 E F G F37 Names of Some Common Organic Compounds F39 Exercises F41 Moles and Molar Masses F42 E.1 E.2 F42 F44 F49 F67 F69 F71 The Mole Molar Mass Exercises F73 I.1 I.2 I.3 I.4 F73 F75 F75 F77 F78 F80 J.1 J.2 J.3 F81 F82 F84 F85 K.3 K.4 L L.1 L.2 Oxidizing and Reducing Agents Balancing Simple Redox Equations Exercises Mole-to-Mole Predictions Mass-to-Mass Predictions F86 F87 F88 F89 F91 F93 F94 F96 F96 F97 TOOLBOX L.1 • How to Carry Out Mass-to-Mass Calculations F97 L.3 F99 Volumetric Analysis TOOLBOX L.2 • How to Interpret a Titration Exercises M Limiting Reactants M.1 M.2 F57 M.3 F57 Oxidation and Reduction Oxidation Numbers: Keeping Track of Electrons Reaction Stoichiometry F51 F53 F54 F56 Classifying Mixtures Acids and Bases in Aqueous Solution Strong and Weak Acids and Bases Neutralization Exercises Redox Reactions F.1 F.2 F.3 Mixtures and Solutions Electrolytes Precipitation Reactions Ionic and Net Ionic Equations Putting Precipitation to Work Exercises Acids and Bases F51 Mass Percentage Composition Determining Empirical Formulas Determining Molecular Formulas Exercises Symbolizing Chemical Reactions Balancing Chemical Equations Exercises Aqueous Solutions and Precipitation Determination of Chemical Formulas G.1 iv F36 F65 H.1 H.2 TOOLBOX K.1 • How to Assign Oxidation Numbers F33 F33 F35 F64 F67 K.1 K.2 F33 F59 F60 F63 Chemical Equations TOOLBOX D.1 • How to Name Ionic Compounds F35 D.4 Separation Techniques Concentration Dilution TOOLBOX G.1 • How to Calculate the Volume of Stock Solution Required for a Given Dilution F1 Chemistry and Society Chemistry: A Science at Three Levels How Science Is Done The Branches of Chemistry Mastering Chemistry A.1 A.2 A.3 G.2 G.3 G.4 xiii Reaction Yield The Limits of Reaction TOOLBOX M.1 • How to Identify the Limiting Reactant Combustion Analysis Exercises F100 F103 F106 F106 F107 F108 F111 F114 FMTOC.indd Page v 11/6/12 5:52 PM user-F393 /Users/user-F393/Desktop Contents Chapter THE QUANTUM WORLD Investigating Atoms 1.1 1.2 1.3 The Nuclear Model of the Atom The Characteristics of Electromagnetic Radiation Atomic Spectra Quantum Theory 1.4 1.5 1.6 1.7 Radiation, Quanta, and Photons The Wave–Particle Duality of Matter The Uncertainty Principle Wavefunctions and Energy Levels BOX 1.1 • Frontiers of Chemistry: Nanocrystals and Fluorescence Microscopy Exercises Chapter QUANTUM MECHANICS IN ACTION: ATOMS The Hydrogen Atom 2.1 2.2 2.3 The Principal Quantum Number Atomic Orbitals Electron Spin Covalent Bonds 9 15 17 19 22 25 31 31 32 33 40 41 2.4 41 Many-Electron Atoms 2.5 2.6 Orbital Energies The Building-Up Principle TOOLBOX 2.1 • How to Predict the GroundState Electron Configuration of an Atom 47 2.7 49 Electronic Structure and the Periodic Table The Periodicity of Atomic Properties 2.8 2.9 2.10 2.11 2.12 2.13 2.14 Atomic Radius Ionic Radius Ionization Energy Electron Affinity The Inert-Pair Effect Diagonal Relationships The General Properties of the Elements Exercises Chapter CHEMICAL BONDS 50 50 52 54 56 58 58 58 61 67 Ionic Bonds 68 3.1 3.2 3.3 3.4 68 70 71 72 The Ions That Elements Form Lewis Symbols The Energetics of Ionic Bond Formation Interactions Between Ions 76 77 TOOLBOX 3.1 • How to Write the Lewis Structure of a Polyatomic Species 78 3.7 3.8 80 83 Resonance Formal Charge TOOLBOX 3.2 • How to Use Formal Charge to Determine the most Likely Lewis Structure Exceptions to the Octet Rule 3.9 Radicals and Biradicals BOX 3.1 • What Has This To Do With Staying Alive? Chemical Self-Preservation 3.10 3.11 3.12 3.13 Expanded Valence Shells The Unusual Structures of Some Group 13 Compounds Correcting the Covalent Model: Electronegativity Correcting the Ionic Model: Polarizability The Strengths and Lengths of Covalent Bonds 3.14 3.15 3.16 Bond Strengths Variation in Bond Strength Bond Lengths BOX 3.2 • How Do We Know The Length of a Chemical Bond? Exercises 42 42 44 76 Lewis Structures Lewis Structures of Polyatomic Species Ionic versus Covalent Bonds BOX 2.1 • How Do We Know That an Electron Has Spin? The Electronic Structure of Hydrogen 3.5 3.6 v 84 85 85 86 87 89 90 90 92 93 93 93 95 97 98 MAJOR TECHNIQUE • Infrared Spectroscopy 105 Exercises Chapter MOLECULAR SHAPE AND STRUCTURE BOX 4.1 • Frontiers of Chemistry: Drugs By Design and Discovery The VSEPR Model 4.1 4.2 The Basic VSEPR Model Molecules with Lone Pairs on the Central Atom 106 107 108 109 109 112 TOOLBOX 4.1 • How to Use the Vsepr Model 115 4.3 117 Polar Molecules Valence-Bond Theory 4.4 4.5 4.6 4.7 Sigma and Pi Bonds Electron Promotion and the Hybridization of Orbitals Other Common Types of Hybridization Characteristics of Multiple Bonds 120 120 122 124 127 FMTOC.indd Page vi 11/6/12 5:52 PM user-F393 /Users/user-F393/Desktop Contents vi Molecular Orbital Theory BOX 4.2 • How Do We Know That Electrons are Not Paired? 4.8 4.9 4.10 Toolbox 4.2 • How to Determine the Electron Configuration and Bond Order of a Homonuclear Diatomic Species 4.12 Bonding in Heteronuclear Diatomic Molecules Orbitals in Polyatomic Molecules Exercises MAJOR TECHNIQUE • Ultraviolet and Visible Spectroscopy Exercises Chapter THE PROPERTIES OF GASES The Nature of Gases 5.1 5.2 5.3 Observing Gases Pressure Alternative Units of Pressure The Gas Laws 5.4 5.5 130 The Limitations of Lewis’s Theory 130 Molecular Orbitals 131 Electron Configurations of Diatomic Molecules 132 BOX 4.3 • How Do We Know The Energies of Molecular Orbitals 4.11 129 The Experimental Observations Applications of the Ideal Gas Law 134 135 137 139 140 146 147 149 Gas Density The Stoichiometry of Reacting Gases Mixtures of Gases Molecular Motion 5.9 5.10 5.11 154 154 157 161 163 165 169 Diffusion and Effusion The Kinetic Model of Gases The Maxwell Distribution of Speeds 169 170 174 BOX 5.1 • How Do We Know The Distribution of Molecular Speeds? 175 Real Gases 176 5.12 5.13 5.14 176 177 178 181 Deviations from Ideality The Liquefaction of Gases Equations of State of Real Gases Exercises Chapter LIQUIDS AND SOLIDS Intermolecular Forces 6.1 6.2 The Origin of Intermolecular Forces Ion–Dipole Forces 6.7 6.8 189 190 190 191 Order in Liquids Viscosity and Surface Tension Solid Structures 192 194 197 198 199 199 199 201 Classification of Solids 201 BOX 6.1 • How Do We Know What a Surface Looks Like? 202 6.10 6.11 6.12 6.13 6.14 Molecular Solids Network Solids Metallic Solids Unit Cells Ionic Structures 203 204 205 207 211 The Impact on Materials 213 6.15 6.16 Liquid Crystals Ionic Liquids Exercises MAJOR TECHNIQUE • X-Ray Diffraction Exercises 150 150 150 152 Dipole–Dipole Forces London Forces Hydrogen Bonding Repulsions Liquid Structure 6.9 TOOLBOX 5.1 • How to Use the Ideal Gas Law 158 5.6 5.7 5.8 6.3 6.4 6.5 6.6 Chapter INORGANIC MATERIALS Metallic Materials 7.1 7.2 7.3 7.4 The Properties of Metals Alloys Steel Nonferrous Alloys Hard Materials 7.5 7.6 7.7 7.8 7.9 7.10 7.11 Diamond and Graphite Calcium Carbonate Silicates Cement and Concrete Borides, Carbides, and Nitrides Glasses Ceramics Materials for New Technologies 7.12 7.13 7.14 7.15 7.16 7.17 Bonding in the Solid State Semiconductors Superconductors Luminescent Materials Magnetic Materials Composite Materials Nanomaterials 7.18 7.19 7.20 The Nature and Uses of Nanomaterials Nanotubes Preparation of Nanomaterials Exercises 214 215 216 223 225 227 228 228 229 231 232 233 233 234 235 237 238 239 240 242 242 244 244 246 248 249 250 250 251 252 255 FMTOC.indd Page vii 11/6/12 5:52 PM user-F393 /Users/user-F393/Desktop Contents Chapter THERMODYNAMICS: THE FIRST LAW Systems, States, and Energy 8.1 8.2 8.3 8.4 8.5 8.6 8.7 Systems Work and Energy Expansion Work Heat The Measurement of Heat The First Law A Molecular Interlude: The Origin of Internal Energy Enthalpy 8.8 8.9 8.10 8.11 8.12 9.7 259 260 260 261 262 267 268 272 276 278 Heat Transfers at Constant Pressure Heat Capacities at Constant Volume and Constant Pressure A Molecular Interlude: The Origin of the Heat Capacities of Gases The Enthalpy of Physical Change Heating Curves BOX 8.1 • How Do We Know The Shape of a Heating Curve? The Enthalpy of Chemical Change 8.13 8.14 8.15 8.16 9.6 Reaction Enthalpies The Relation Between ⌬H and ⌬U Standard Reaction Enthalpies Combining Reaction Enthalpies: Hess’s Law 286 287 287 289 291 292 TOOLBOX 8.1 • How to Use Hess’s Law 292 8.17 8.18 8.19 8.20 294 298 300 Standard Enthalpies of Formation The Born–Haber Cycle Bond Enthalpies The Variation of Reaction Enthalpy with Temperature BOX 8.2 • What Has This To Do With The Environment? Alternative Fuels The Impact on Technology 8.21 The Heat Output of Reactions Exercises 336 9.8 339 302 304 304 305 308 Standard Reaction Entropies Global Changes in Entropy 9.9 9.10 9.11 The Surroundings The Overall Change in Entropy Equilibrium Gibbs Free Energy 9.12 9.13 9.14 9.15 280 283 285 Focusing on the System Gibbs Free Energy of Reaction The Gibbs Free Energy and Nonexpansion Work The Effect of Temperature Impact on Biology 9.16 Gibbs Free Energy Changes in Biological Systems Exercises Chapter 10 PHYSICAL EQUILIBRIA Phases and Phase Transitions 10.1 10.2 10.3 10.4 10.5 10.6 10.7 Vapor Pressure Volatility and Intermolecular Forces The Variation of Vapor Pressure with Temperature Boiling Freezing and Melting Phase Diagrams Critical Properties Solubility 10.8 10.9 10.10 10.11 10.12 10.13 Entropy 9.1 9.2 9.3 9.4 9.5 Spontaneous Change Entropy and Disorder Changes in Entropy Entropy Changes Accompanying Changes in Physical State A Molecular Interpretation of Entropy 10.14 317 Molality 341 343 346 347 348 351 355 356 358 358 360 367 368 368 369 369 373 374 375 378 380 381 382 383 384 386 388 388 TOOLBOX 10.1 • How to Use the Molality 389 10.15 10.16 392 Vapor-Pressure Lowering Boiling-Point Elevation and Freezing-Point Depression Osmosis 317 10.17 318 318 320 TOOLBOX 10.2 • How to Use Colligative Properties to Determine Molar Mass Binary Liquid Mixtures 326 330 340 380 The Limits of Solubility The Like-Dissolves-Like Rule Pressure and Gas Solubility: Henry’s Law Temperature and Solubility The Enthalpy of Solution The Gibbs Free Energy of Solution Colligative Properties Chapter THERMODYNAMICS: THE SECOND AND THIRD LAWS 333 335 BOX 9.1 • Frontiers of Chemistry: The Quest for Absolute Zero 278 279 The Equivalence of Statistical and Thermodynamic Entropies Standard Molar Entropies vii 10.18 The Vapor Pressure of a Binary Liquid Mixture 394 397 399 402 402 FMTOC.indd Page viii 10/18/12 8:07 PM user-F393 viii /Users/user-F393/Desktop Contents 10.19 10.20 Distillation Azeotropes The Impact on Biology and Materials 10.21 10.22 Colloids Bio-Based and Biomimetic Materials BOX 10.1 • Frontiers of Chemistry: Drug Delivery Exercises MAJOR TECHNIQUE • Chromatography Exercises 404 406 407 408 409 12.10 The pH of Solutions of Weak Acids and Bases 12.11 Reactions at Equilibrium 11.1 11.2 11.3 11.4 11.5 The Reversibility of Reactions Equilibrium and the Law of Mass Action The Thermodynamic Origin of Equilibrium Constants The Extent of Reaction The Direction of Reaction Equilibrium Calculations 11.6 11.7 11.8 The Equilibrium Constant in Terms of Molar Concentrations of Gases Alternative Forms of the Equilibrium Constant Using Equilibrium Constants TOOLBOX 11.1 • How to Set Up and Use an Equilibrium Table The Response of Equilibria to Changes in Conditions 11.9 11.10 11.11 Adding and Removing Reagents Compressing a Reaction Mixture Temperature and Equilibrium Impact on Materials and Biology 11.12 11.13 Catalysts and Haber’s Achievement Homeostasis Exercises Solutions of Weak Acids The Nature of Acids and Bases 12.1 12.2 12.3 12.4 12.5 12.6 Brønsted–Lowry Acids and Bases Lewis Acids and Bases Acidic, Basic, and Amphoteric Oxides Proton Exchange Between Water Molecules The pH Scale The pOH of Solutions Weak Acids and Bases 12.7 12.8 12.9 Acidity and Basicity Constants The Conjugate Seesaw Molecular Structure and Acid Strength 485 486 TOOLBOX 12.1 • How to Calculate the pH of a Solution of a Weak Acid 486 411 12.12 419 TOOLBOX 12.2 • How to Calculate the pH of a Solution of a Weak Base 489 420 Solutions of Weak Bases The pH of Salt Solutions Polyprotic Acids and Bases 421 422 422 424 427 433 435 436 12.14 12.15 12.16 The pH of a Polyprotic Acid Solution Solutions of Salts of Polyprotic Acids The Concentrations of Solute Species 491 496 496 497 499 500 12.17 503 Composition and pH BOX 12.1 • What Has This To Do With The Environment? Acid Rain and the Gene Pool Autoprotolysis and pH 436 439 440 489 TOOLBOX 12.3 • How to Calculate the Concentrations of all Species in a Polyprotic Acid Solution 12.18 12.19 Very Dilute Solutions of Strong Acids and Bases Very Dilute Solutions of Weak Acids Exercises 504 506 507 508 511 440 445 445 448 450 453 453 454 455 Chapter 13 AQUEOUS EQUILIBRIA Mixed Solutions and Buffers 13.1 13.2 13.3 Buffer Action Designing a Buffer Buffer Capacity BOX 13.1 • What Has This To Do With Staying Alive? Physiological Buffers Titrations Chapter 12 ACIDS AND BASES 482 410 12.13 Chapter 11 CHEMICAL EQUILIBRIA The Strengths of Oxoacids and Carboxylic Acids 13.4 463 463 464 467 468 469 471 474 475 476 478 480 519 520 520 521 527 528 529 Strong Acid–Strong Base Titrations 529 TOOLBOX 13.1 • How to Calculate the pH During a Strong Acid–Strong Base Titration 530 13.5 Strong Acid–Weak Base and Weak Acid–Strong Base Titrations 532 TOOLBOX 13.2 • How to Calculate the pH During a Titration of a Weak Acid or a Weak Base 535 13.6 13.7 537 539 Acid–Base Indicators Stoichiometry of Polyprotic Acid Titrations Solubility Equilibria 13.8 13.9 The Solubility Product The Common-Ion Effect 541 541 544 c02QuantumMechanicsInActionAtoms.indd Page 44 6/21/12 4:06 PM user-F393 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms 44 FIGURE 2.15 The radial distribution functions for s-, p-, and d-orbitals in the first three shells of a hydrogen atom Note that the probability maxima for orbitals of the same shell are close to each other; however, note also that an electron in an ns-orbital has a higher probability of being found close to the nucleus than does an electron in an np-orbital or an nd-orbital 0.6 0.5 1s The effects of penetration and shielding can be large A 4s-electron generally has a much lower energy than that of a 4p- or 4d-electron; it may even have lower energy than that of a 3d-electron of the same atom (see Fig 2.14) The precise ordering of orbitals depends on the number of electrons in the atom, as we shall see in the next section 0.4 Radial distribution function, P(r)a0 0.3 In a many-electron atom, because of the effects of penetration and shielding, the order of energies of orbitals in a given shell is s Ͻ p Ͻ d Ͻ f 0.2 2s 2.6 The Building-Up Principle 0.1 The electronic structure of an atom determines its chemical properties, and so we need to be able to describe that structure To so, we write the electron configuration of the atom—a list of all its occupied orbitals, with the numbers of electrons that occupy each one In the ground state of a many-electron atom, the electrons occupy atomic orbitals in such a way that the total energy of the atom is a minimum At first sight, we might expect an atom to have its lowest energy when all its electrons are in the lowest-energy orbital (the 1s-orbital) However, except for hydrogen and helium, which have no more than two electrons, that can never happen In 1925, the Austrian scientist Wolfgang Pauli discovered a general and very fundamental rule about electrons and orbitals that is now known as the Pauli exclusion principle: 3s 0.2 2p 0.1 3p No more than two electrons may occupy any given orbital When two electrons occupy one orbital, their spins must be paired 0.2 3d 0.1 0 10 20 Radius, r/a0 30 1s H 1s1 1s He 1s2 The spins of two electrons are said to be paired if one is c and the other T (FIG 2.16) Paired spins are denoted cT , and electrons with paired spins have spin magnetic quantum numbers of opposite sign Because an atomic orbital is designated by three quantum numbers (n, l, and ml) and the two spin states are specified by a fourth quantum number, ms, another way of expressing the Pauli exclusion principle for atoms is No two electrons in an atom can have the same set of four quantum numbers The exclusion principle implies that each atomic orbital can hold no more than two electrons The hydrogen atom in its ground state has one electron in the 1s-orbital To show this structure, we place a single arrow in the 1s-orbital in a “box diagram,” which shows each orbital as a box that can be occupied by no more than two electrons (see diagram 1, which is a fragment of Fig 2.14) We then report its configuration as 1s1 (“one s one”) In the ground state of a helium (He) atom (Z ϭ 2), both electrons are in a 1s-orbital, which is reported as 1s2 (“one s two”) As we see in (2), the two electrons are paired At this point, the 1s-orbital and the shell with n ϭ are fully occupied We say that the helium atom has a closed shell, a shell containing the maximum number of electrons allowed by the exclusion principle A Note on Good Practice: When a single electron occupies an orbital, write 1s1, for instance, not simply 1s ■ The outermost electrons are used in the formation of chemical bonds (Chapter 3), and the theory of bond formation is called valence theory— hence the name of these electrons Lithium (Z ϭ 3) has three electrons Two electrons occupy the 1s-orbital and complete the n ϭ shell The third electron must occupy the next available orbital up the ladder of energy levels, the 2s-orbital (see Fig 2.14) The ground state of a lithium (Li) atom is therefore 1s22s1 (3) We can think of the electronic structure of an atom as having an inner core consisting of the electrons in filled orbitals, surrounded by the valence electrons, the electrons in the outermost shell In the case of lithium the core is made up of the inner heliumlike closed shell, the 1s2 core, which c02QuantumMechanicsInActionAtoms.indd Page 45 6/21/12 4:06 PM user-F393 /Users/user-F393/Desktop 2.6 The Building-Up Principle we denote [He] The core is surrounded by an outer shell containing a higher-energy 2s-electron Therefore, the electron configuration of lithium is [He]2s1 In general, only valence electrons can be lost in chemical reactions, because core electrons are in lower-energy orbitals and so are too tightly bound Thus, lithium loses only one electron when it forms compounds; it forms Liϩ ions, rather than Li2ϩ or Li3ϩ ions The element with Z ϭ is beryllium (Be), with four electrons The first three electrons form the configuration 1s22s1, like lithium The fourth electron pairs with the 2s-electron, giving the configuration 1s22s2, or, more simply, [He]2s2 (4) A beryllium atom therefore has a heliumlike core surrounded by a valence shell of two paired electrons Like lithium, and for the same reason, a Be atom can lose only its valence electrons in chemical reactions Thus, it loses both 2s-electrons to form a Be2ϩ ion Boron (Z ϭ 5) has five electrons Two enter the 1s-orbital and complete the n ϭ shell Two enter the 2s-orbital The fifth electron occupies an orbital of the next available subshell, which Fig 2.14 shows is a 2p-orbital This arrangement of electrons is reported as the configuration 1s22s22p1 or [He]2s22p1 (5), showing that boron has three valence electrons around a heliumlike core We need to make another decision at carbon (Z ϭ 6): does the sixth electron join the one already in the 2p-orbital, or does it enter a different 2p-orbital? (Remember, there are three p-orbitals in the subshell, all of the same energy.) To answer this question, we note that electrons are farther from each other and repel each other less when they occupy different p-orbitals than when they occupy the same orbital So the sixth electron goes into an empty 2p-orbital, and the ground state of carbon is 1s22s22px12py1 (6) We write out the individual orbitals like this only when we need to emphasize that electrons occupy different orbitals within a subshell In most cases, we can write the shorter form, [He]2s22p2 Note that in the orbital diagram we have drawn the two 2p-electrons with parallel spins ( c c), indicating that they have the same spin magnetic quantum numbers For reasons based in quantum mechanics, electrons with parallel spins tend to avoid each other Therefore, this arrangement has slightly lower energy than that of a paired arrangement However, it is allowed only when the electrons occupy different orbitals The procedure that we have been using is called the building-up principle It can be summarized by two rules To predict the ground-state configuration of a neutral atom of an element with atomic number Z with its Z electrons: Add Z electrons, one after the other, to the orbitals in the order shown in FIG 2.17 but with no more than two electrons in any one orbital If more than one orbital in a subshell is available, add electrons with parallel spins to different orbitals of that subshell rather than pairing two electrons in one of the orbitals The first rule takes into account the Pauli exclusion principle The second rule is called Hund’s rule, for the German spectroscopist Friedrich Hund, who first proposed it (a) (b) FIGURE 2.16 (a) Two electrons are said to be paired if they have opposite spins (one clockwise, the other counterclockwise) (b) Two electrons are classified as having parallel spins if their spins are in the same direction—in this case, both c 2s 1s Li 1s22s1, [He]2s1 2s 1s Be 1s22s2, [He]2s2 2p 2s 1s B 1s22s22p1, [He]2s22p1 2p 2s 1s C 1s22s22p2, [He]2s22p2 The building-up principle is also commonly called the Aufbau principle, from the German word for “building up.” Start H 1s s-block f-block d-block p-block He [He] 2s 2p Ne [Ne] 3s 3p Ar [Ar] 4s 3d 4p Kr [Kr] 5s 4d 5p Xe [Xe] 6s 5d 4f 6p Rn [Rn] 7s 6d 5f 7p 14 10 45 FIGURE 2.17 The names of the blocks of the periodic table indicate the last subshell being occupied according to the building-up principle The numbers of electrons that each type of orbital can accommodate are shown by the numbers across the bottom of the table The colors of the blocks match the colors that we are using for the corresponding orbitals c02QuantumMechanicsInActionAtoms.indd Page 46 6/21/12 4:06 PM user-F393 46 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms 2p 2s 1s N 1s22s22p3, [He]2s22p3 2p 2s 1s This procedure gives the configuration of the atom that corresponds to the lowest total energy, which maximizes the attraction of the electrons to the nucleus and minimizes their repulsion by one another An atom with electrons in energy states higher than predicted by the building-up principle is said to be in an excited state For example, the electron configuration [He]2s12p3 represents an excited state of a carbon atom An excited state is unstable and emits a photon as the electron returns to an orbital that restores the atom to a lower energy In general, an atom of any element has a noble-gas core surrounded by a number of electrons in the valence shell, the outermost occupied shell The valence shell is the occupied shell with the largest value of n The underlying organization of the periodic table described in Fundamentals, Section B, now begins to unfold All the atoms of the main-group elements in a given period have a valence shell with the same principal quantum number, which is equal to the period number For example, the valence shell of elements in Period (from lithium to neon) is the shell with n ϭ Thus all the atoms in a given period have the same type of core and different numbers of valence electrons with the same principal quantum number For example, the atoms of Period elements all have a heliumlike 1s2 core, denoted [He], and those of Period elements have a neonlike 1s22s22p6 core, denoted [Ne] All the atoms of a given group (in the main groups, particularly) have analogous valence electron configurations that differ only in the value of n For instance, all the members of Group have the valence configuration ns1; and all the members of Group 14 have the valence configuration ns2np2 These similar electron configurations give the elements in a group similar chemical properties, as illustrated in Fundamentals, Section B With these points in mind, let’s continue building up the electron configurations across Period Nitrogen has Z ϭ and one more electron than carbon, giving [He]2s22p3 Each p-electron occupies a different orbital, and the three have parallel spins (7) Oxygen has Z ϭ and one more electron than nitrogen; therefore, its configuration is [He]2s22p4 (8) and two of its 2p-electrons are paired Similarly, fluorine, with Z ϭ and one more electron than oxygen, has the configuration [He]2s22p5 (9), with only one unpaired electron Neon, with Z ϭ 10, has one more electron than fluorine This electron completes the 2p-subshell, giving [He]2s22p6 (10) According to Figs 2.14 and 2.17, the next electron enters the 3s-orbital, the lowest-energy orbital of the next shell The configuration of sodium is therefore [He]2s22p63s1, or, more briefly, [Ne]3s1, where [Ne] denotes the neonlike core Self-Test 2.3A Predict the ground-state configuration of a magnesium atom O 1s22s22p4, [He]2s22p4 [Answer: 1s22s22p63s2, or [Ne]3s2] 2p Self-Test 2.3B Predict the ground-state configuration of an aluminum atom ■ 2s The s- and p-orbitals of the shell with n ϭ are full by the time we get to argon, [Ne]3s23p6, which is a colorless, odorless, unreactive gas resembling neon Argon completes the third period From Fig 2.14, we see that the energy of the 4s-orbital is slightly lower than that of the 3d-orbitals As a result, instead of electrons entering the 3d-orbitals, the fourth period now begins by filling the 4s-orbitals (see Fig 2.14) Hence, the next two electron configurations are [Ar]4s1 for potassium and [Ar]4s2 for calcium, where [Ar] denotes the argonlike 1s22s22p63s23p6 core At this point, however, the 3d-orbitals begin to be occupied, and there is a change in the rhythm of the periodic table According to the pattern of increasing energy of the orbitals (see Fig 2.14), the next 10 electrons (for scandium, with Z ϭ 21, through zinc, with Z ϭ 30) enter the 3d-orbitals The ground-state electron configuration of scandium, for example, is [Ar]3d14s2, and that of its neighbor titanium is [Ar]3d24s2 Note that, beginning at scandium, we write the 4s-electrons after the 3d-electrons: once they contain electrons, the 3d-orbitals lie lower in energy than the 4s-orbital (recall Fig 2.14; the same relation holds true for nd- and (n ϩ 1)s-orbitals in subsequent periods) Successive electrons are added to the d-orbitals as Z increases However, there are two exceptions: the experimental electron configuration of chromium is [Ar]3d54s1 instead of [Ar]3d44s2, and 1s F 1s22s22p5, [He]2s22p5 2p 2s 1s 10 Ne 1s22s22p6, [He]2s22p6 c02QuantumMechanicsInActionAtoms.indd Page 47 5/25/12 9:28 PM user-F393 /Users/user-F393/Desktop 2.6 The Building-Up Principle 47 that of copper is [Ar]3d104s1 instead of [Ar]3d94s2 This apparent discrepancy occurs because the half-complete subshell configuration d5 and the complete subshell configuration d10 turn out to have lower energy than simple theory suggests As a result, a lower total energy may be achieved if an electron enters a 3d-orbital instead of the expected 4s-orbital, if that arrangement completes a half-subshell or a full subshell Other exceptions to the building-up principle can be found in the complete listing of electron configurations in Appendix 2C and in the periodic table inside the front cover As we can anticipate from the structure of the periodic table (see Fig 2.17), electrons occupy 4p-orbitals once the 3d-orbitals are full The configuration of germanium, [Ar]3d104s24p2, for example, is obtained by adding two electrons to the 4p-orbitals outside the completed 3d-subshell Arsenic has one more electron and the configuration [Ar]3d104s24p3 The fourth period of the table contains 18 elements, because the 4s- and 4p-orbitals together can accommodate a total of electrons and the 3d-orbitals can accommodate 10 Period is the first long period of the periodic table THINKING POINT At approximately what value of atomic number might an “extra-long period,” corresponding to the filling of g-orbitals, appear, and how long would it be? Next in line for occupation at the beginning of Period is the 5s-orbital, followed by the 4d-orbitals As in Period 4, the energies of the 4d-orbitals fall below that of the 5s-orbital after two electrons have been accommodated in the 5s-orbital A similar effect is seen in Period 6, but now another set of inner orbitals, the 4f-orbitals, begins to be occupied Cerium, for example, has the configuration [Xe]4f15d16s2 Electrons then continue to occupy the seven 4f-orbitals, which are complete after 14 electrons have been added, at ytterbium, [Xe]4f146s2 Next, the 5d-orbitals are occupied The 6p-orbitals are occupied only after the 6s-, 4f-, and 5d-orbitals are filled at mercury; thallium, for example, has the configuration [Xe]4f145d106s26p1 You may notice in Appendix 2C several apparent disruptions in the order in which the 4f orbitals are filled The apparent exceptions result because the 4f and 5d orbitals are very close in energy In fact, closely spaced energy levels account for the fact that about 25% of the elements have electron configurations that deviate in some way from these rules However, for the majority of elements the rules are useful guidelines and a good starting point for them all; TOOLBOX 2.1 outlines a procedure for writing the electron configuration of a heavy element Toolbox 2.1 HOW TO PREDICT THE GROUND-STATE ELECTRON CONFIGURATION OF AN ATOM CONCEPTUAL BASIS Electrons occupy orbitals in such a way as to minimize the total energy of an atom by maximizing attractions and minimizing repulsions in accordance with the Pauli exclusion principle and Hund’s rule PROCEDURE Use the following rules of the building-up principle to assign a ground-state configuration to a neutral atom of an element with atomic number Z: Note from the periodic table in which period and group the element is found Its core configuration will be that of the preceding noble-gas configuration together with any completed d- and f-subshells The period number gives the value of the principal quantum number of the valence shell, and the group number is used to find the number of valence electrons Add Z electrons, one after the other, to the orbitals in the order shown in Figs 2.14 and 2.17 but with no more than two electrons in any one orbital (the Pauli exclusion principle) If more than one orbital in a subshell is available, add electrons to different orbitals of the subshell before doubly occupying any of them (Hund’s rule) Write the labels of the orbitals in order of increasing energy, with a superscript that gives the number of electrons in that orbital The configuration of a filled shell is represented by the symbol of the noble gas having that configuration, as in [He] for 1s2 In most cases this procedure gives the ground-state electron configuration of an atom, the arrangement with the lowest energy Any arrangement other than the ground state corresponds to an excited state of the atom Note that we can use the structure of the periodic table to predict the electron configurations of most elements once we realize which orbitals are being filled in each block of the periodic table (see Fig 2.17) Example 2.2 shows how these rules are applied c02QuantumMechanicsInActionAtoms.indd Page 48 5/25/12 7:19 PM user-F393 48 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms EXAMPLE 2.2 Predicting the ground-state electron configuration of a heavy atom Inorganic chemists often develop new compounds after thinking about the location of an element in the periodic table and its valence electron configuration Suppose you are working in a laboratory developing catalysts for an industrial process Predict the ground-state electron configuration of (a) a vanadium atom and (b) a lead atom ANTICIPATE Because vanadium is a member of the d-block, you should expect its atoms to have a partially filled set of d-orbitals Because lead is in the same group as carbon, you should expect the configuration of its valence electrons to be similar to that of carbon (ns2np2) PLAN Follow the procedure in Toolbox 1.1 SOLVE (a) Step Note from the periodic table in which period and group the element is found Its core configuration will be that of the preceding noble-gas configuration together with any completed d- and f-subshells The period number gives the value of the principal quantum number of the valence shell and the group number gives the number of valence electrons Vanadium is in Period and Group 5, and so it has an argon core with five valence electrons Step Add Z electrons, one after the other, to the orbitals in the order shown in Figs 2.14 and 2.17 but with no more than two electrons in any one orbital Step Add two electrons to the 4s-orbital, and the last three electrons to three separate 3d-orbitals Step Write the labels of the orbitals in order of increasing energy Ar K Ca Sc s1 s2 Ti V d1s2 d2s2 d3s2 4s 3d [Ar ]3d34s2 (b) Step As before, find the period and group of the element in the periodic table Lead belongs to Period and Group 14 It has a xenon core with complete 5d- and 4f-subshells and four additional valence electrons Step Add Z electrons, one after the other, to the orbitals in the order shown in Figs 2.14 and 2.17 but with no more than two electrons in any one orbital Step Lead has two valence electrons in a 6s-orbital and two in different 6p-orbitals Step Write the labels of the orbitals in order of increasing energy [Xe ]4f145d106s26p2 C Si Ge Sn Pb 6p 6s EVALUATE As expected, vanadium has an incomplete set of d-electrons and the valence-shell configuration of lead is analogous to that of carbon Self-Test 2.4A Write the ground-state configuration of a bismuth atom [Answer: [Xe]4f145d106s26p3] Self-Test 2.4B Write the ground-state configuration of an arsenic atom Related Exercises 2.43, 2.44 c02QuantumMechanicsInActionAtoms.indd Page 49 5/25/12 7:19 PM user-F393 /Users/user-F393/Desktop 2.7 Electronic Structure and the Periodic Table The ground-state electron configuration of an atom is predicted by using the building-up principle in conjunction with Fig 2.14, the Pauli exclusion principle, and Hund’s rule 2.7 Electronic Structure and the Periodic Table The periodic table is one of the most notable achievements in chemistry because it helps to organize what would otherwise be a bewildering array of properties of the elements However, the fact that its structure corresponds to the electronic structure of atoms was unknown to its discoverers The periodic table was developed solely from a consideration of physical and chemical properties of the elements In 1869 two scientists, the German Lothar Meyer and the Russian Dmitri Mendeleev (FIG 2.18), discovered independently that the elements fall into families with similar properties when they were arranged in order of increasing atomic mass Mendeleev called this observation the periodic law Mendeleev’s chemical insight led him to leave gaps for elements that would be needed to complete the pattern but were unknown at the time When they were discovered later, he turned out (in most cases) to be strikingly correct For example, his pattern required an element that he named “eka-silicon” below silicon and between gallium and arsenic He predicted that the element would have a relative atomic mass of 72 (taking the mass of hydrogen as 1) and properties similar to those of silicon This prediction spurred the German chemist Clemens Winkler in 1886 to search for eka-silicon, which he eventually discovered and named germanium It has a relative atomic mass of 72.59 and properties similar to those of silicon One problem with Mendeleev’s table was that some elements seemed to be out of place For example, when argon was isolated, it did not seem to have the correct mass for its location Its relative atomic mass of 40 is the same as that of calcium, but argon is an inert gas and calcium is a reactive metal Such anomalies led scientists to question the use of relative atomic mass as the basis for organizing the elements When Henry Moseley examined x-ray spectra of the elements in the early twentieth century, he realized that he could infer the atomic number itself It was soon discovered that elements fall into the uniformly repeating pattern of the periodic table if they are organized according to atomic number rather than atomic mass At the time that the periodic table was formulated, the reason for the periodicity of the elements was a mystery Now, however, we can understand the organization of the periodic table in terms of the electron configurations of the elements The table is divided into s-, p-, d-, and f-blocks, named for the last subshell that is occupied according to the building-up principle (as shown in Fig 2.17) Two elements are exceptions Because it has two 1s-electrons, we would place helium in the s-block, but it is shown in the p-block because of its properties: it is a gas with properties closely matching those of the noble gases in Group 18, rather than the reactive metals in Group Its place in Group 18 is justified because it has a filled valence shell, like all the other Group 18 elements Hydrogen occupies a unique position in the periodic table It has one s-electron, and so it belongs in Group 1; but it is also one electron short of a noble-gas configuration, and so it can act like a member of Group 17 Because hydrogen has such a unique character, we not ascribe it to any group; however, you will often see it placed in Group or Group 17, and sometimes in both THINKING POINT What are the arguments for and against including He in Group 2, above beryllium? The s- and p-blocks form the main groups of the periodic table The similar valence-shell electron configurations for the elements in the same main group are the reason for the similar properties of these elements The group number tells us how many valence-shell electrons are present In the s-block, the group number (1 or 2) is the same as the number of valence electrons This relation is also true for all main groups when the older practice of using Roman numerals (I–VIII) to label (a) (b) FIGURE 2.18 (a) Dmitri Ivanovitch Mendeleev (1834–1907) and (b) Lothar Meyer (1830–1895) 49 c02QuantumMechanicsInActionAtoms.indd Page 50 5/25/12 7:19 PM user-F393 50 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms the groups is used However, when the group labels 1–18 are used, in the p-block we subtract 10 from the group number to find the number of valence electrons For example, fluorine in Group 17 (old notation: Group VII) has seven valence electrons Each new period corresponds to the occupation of a shell with a higher principal quantum number This correspondence explains the different lengths of the periods Period consists of only two elements, H and He, in which the single 1s-orbital of the n ϭ shell is being filled with its two electrons Period consists of the eight elements Li through Ne, in which the one 2s- and three 2p-orbitals are being filled with eight more electrons In Period (Na through Ar), the 3s- and 3p-orbitals are being occupied by eight additional electrons In Period 4, not only are the eight electrons of the 4s- and 4p-orbitals being added, so are the ten electrons of the 3d-orbitals Hence there are 18 elements in Period Period elements add another 18 electrons as the 5s-, 4d-, and 5p-orbitals are filled In Period 6, a total of 32 electrons are added, because 14 electrons are also being added to the seven 4f-orbitals The f-block elements have very similar chemical properties, because their electron configurations differ only in the population of inner f-orbitals, and electrons in these orbitals not participate much in bond formation The blocks of the periodic table are named for the last orbital to be occupied according to the building-up principle The periods are numbered according to the principal quantum number of the valence shell The Periodicity of Atomic Properties The periodic table can be used to predict a wide range of properties, many of which are crucial for understanding chemistry The variation of effective nuclear charge through the periodic table plays an important role in the explanation of periodic trends FIGURE 2.19 shows the variation for the first three periods The effective charge increases from left to right across a period and falls back sharply upon going to the next period THINKING POINT Before reading further, predict how the effective nuclear charge might affect some atomic properties, such as the size of an atom or the ease with which an outer electron can be removed 2.8 Atomic Radius Electron clouds not have sharp boundaries, and so we cannot measure the exact radius of an atom However, when atoms pack together in solids and bond Ar Cl FIGURE 2.19 The variation of the effective nuclear charge for the outermost valence electron with atomic number Notice that the effective nuclear charge increases from left to right across a period but drops when the outer electrons occupy a new shell (The effective nuclear charge is actually Zeffe, but Zeff itself is commonly referred to as the charge.) Effective nuclear charge, Zeff Ne S F P O Mg C Na B Si Al N Be He Li 11 13 Atomic number, Z 15 17 c02QuantumMechanicsInActionAtoms.indd Page 51 6/7/12 8:52 PM user-F393 /Users/user-F393/Desktop 2.8 Atomic Radius together to form molecules, their centers are found at definite distances from one another The atomic radius of an element is defined as half the distance between the centers of neighboring atoms (11) If the element is a metal, its atomic radius is taken to be half the distance between the centers of neighboring atoms in a solid sample For instance, because the distance between neighboring nuclei in solid copper is 256 pm, the atomic radius of copper is 128 pm If the element is a nonmetal or a metalloid, we use half the distance between the nuclei of atoms joined by a chemical bond; this radius is also called the covalent radius of the element, for reasons that will become clear in Chapter For instance, the distance between the nuclei in a Cl2 molecule is 198 pm, and so the covalent radius of chlorine is 99 pm If the element is a noble gas, we use the van der Waals radius, which is half the distance between the centers of neighboring atoms in a sample of the solidified gas The atomic radii of the noble gases listed in Appendix 2D are all van der Waals radii Because the atoms in a sample of a noble gas are not chemically bonded together, van der Waals radii are generally much larger than covalent radii and are best not included in the discussion of trends FIGURE 2.20 shows some atomic radii, and FIG 2.21 shows the variation in atomic radius with atomic number Note the periodic, sawtooth pattern in the latter plot A feature to note is that: 51 2r 11 Atomic radius • Atomic radius generally decreases from left to right across a period and increases down a group The increase down a group, such as that from Li to Cs, makes sense: with each new period, the outermost electrons occupy shells with increasing principal quantum 13 14 15 16 17 18 Li 152 Be 113 B 88 C 77 N 75 O 66 F 58 Ne Na 154 Mg 160 Al 143 Si 117 P 110 S 104 Cl 99 Ar K 227 Ca 197 Ga 122 Ge 122 As 121 Se 117 Br 114 Kr Rb 248 Sr 215 In 163 Sn 141 Sb 141 Te 137 I 133 Xe Tl 170 Pb 175 Bi 155 Po 167 At Rn Ba 217 Cs 265 Cs 300 Rb K Atomic radius (pm) FIGURE 2.20 The atomic radii (in picometers) of the main-group elements The radii decrease from left to right in a period and increase down a group The colors used here and in subsequent charts represent the general magnitude of the property Atomic radii, including those of the d-block elements, are listed in Appendix 2D Na 200 Po Li I Br Cl 100 F Atomic number FIGURE 2.21 The periodic variation in the atomic radii of the elements The decrease across a period can be explained in terms of the effect of increasing effective nuclear charge, the increase down a group by the occupation of shells with increasing principal quantum number c02QuantumMechanicsInActionAtoms.indd Page 52 6/21/12 4:06 PM user-F393 52 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms number and therefore lie farther from the nucleus The decrease across a period, such as that from Li to Ne, is surprising at first, because the number of electrons is increasing along with the number of protons The explanation is that the new electrons are in the same shell of the atom and about as close to the nucleus as other electrons in the same shell However, because they are spread out, the electrons not shield one another well from the nuclear charge; so the effective nuclear charge increases across the period The increasing effective nuclear charge draws the electrons in, and, as a result, the atom is more compact and we see a diagonal trend for atomic radii to increase from the upper right of the periodic table to the lower left THINKING POINT Which currently known element has the biggest atoms? Atomic radii generally decrease from left to right across a period as the effective atomic number increases, and they increase down a group as successive shells are occupied 2.9 Ionic Radius ranion ϩ rcation Ϫ 12 Ionic radius ϩ The radii of ions differ markedly from the radii of their parent atoms As described in Fundamentals, Section C, in an ionic solid each ion is surrounded by ions with the opposite charge The ionic radius of an element is its share of the distance between neighboring ions in an ionic solid (12) The distance between the centers of a neighboring cation and anion is the sum of the two ionic radii In practice, we take the radius of the oxide ion to be 140 pm and calculate the radii of other ions on the basis of that value For example, because the distance between the centers of neighboring Mg2ϩ and O2Ϫ ions in magnesium oxide is 212 pm, the radius of the Mg2ϩ ion is reported as 212 pm Ϫ 140 pm ϭ 72 pm FIGURE 2.22 illustrates the trends in ionic radii, and FIG 2.23 shows the relative sizes of some ions and their parent atoms All cations are smaller than their parent atoms, because the atom loses one or more electrons to form the cation and exposes its core, which is generally much smaller than the parent atom For example, the atomic radius of Li, with the configuration 1s22s1, is 152 pm, but the ionic radius of Liϩ, the bare heliumlike 1s2 core of the parent atom, is only 76 pm This size difference is comparable to that between a cherry and its pit Atoms in the same main group tend to form ions with the same charge Like atomic radii, the radii of these ions increase down each group because electrons are occupying shells with higher principal quantum numbers Figure 2.23 shows that anions are larger than their parent atoms The reason can be traced to the increased number of electrons in the valence shell of the anion and the repulsive effects exerted by electrons on one another The variation in the 13 Be2ϩ Liϩ 76 Naϩ 102 Kϩ 138 Ca2ϩ 100 Rbϩ 152 Sr2ϩ 118 Csϩ 167 Ba2ϩ 135 45 Mg2ϩ 72 B3ϩ 23 14 15 16 17 18 C N3Ϫ 171 O2Ϫ 140 FϪ 133 Ne Si P3Ϫ 212 S2Ϫ 184 ClϪ 181 Ar Ge As3Ϫ 222 Se2Ϫ 198 BrϪ 196 Kr Sn Sb Te2Ϫ 221 IϪ 220 Xe Pb Bi Po At Rn Al3ϩ 54 Ga3ϩ 62 In3ϩ 80 Tl3ϩ 89 FIGURE 2.22 The ionic radii (in picometers) of the ions of the main-group elements Note that cations are typically smaller than their parent atoms, whereas anions are larger—in some cases, very much larger c02QuantumMechanicsInActionAtoms.indd Page 53 6/21/12 4:06 PM user-F393 /Users/user-F393/Desktop 2.9 Ionic Radius radii of anions shows the same diagonal trend as that for atoms and cations, with the smallest at the upper right of the periodic table, close to fluorine: Liϩ Li Be Be2ϩ • Cations are smaller than their parent atoms, whereas anions are larger Atoms and ions with the same number of electrons are called isoelectronic For example, Naϩ, FϪ, and Mg2ϩ are isoelectronic All three ions have the same electron configuration, [He]2s22p6, but their radii differ because they have different nuclear charges (see Fig 2.22) The Mg2ϩ ion has the largest nuclear charge, so it has the strongest attraction for the electrons and therefore the smallest radius The FϪ ion has the lowest nuclear charge of the three isoelectronic ions and, as a result, it has the largest radius Naϩ Na Mg Mg2ϩ O O2Ϫ F EXAMPLE 2.3 Deciding the relative sizes of ions Mineralogists and geologists often need to identify the relative sizes of atoms to judge whether one mineral might be modified by the inclusion of “alien” ions For example, the different colors of gemstones result from this type of insertion Arrange each of the following pairs of ions in order of increasing ionic radius: (a) Mg2ϩ and Ca2ϩ; (b) O2Ϫ and FϪ PLAN The smaller member of a pair of isoelectronic ions in the same period will be an ion of an element that lies farther to the right in a period, because that ion has the greater effective nuclear charge If the two ions are in the same group, the smaller ion will be the one that lies higher in the group, because its outermost electrons are closer to the nucleus SOLVE (a) Mg lies above Ca in Group 2ϩ Mg has the smaller ionic radius 2؉ Mg 72 pm p 2؉ Ca 100 pm (b) F lies to the right of O in Period FϪ has the smaller ionic radius 15 16 17 2؊ ؊ O F 140 pm 53 133 pm EVALUATE Appendix 2D shows that the actual values are (a) 72 pm for Mg2ϩ and 100 pm for Ca2ϩ; (b) 133 pm for FϪ and 140 pm for O2Ϫ Self-Test 2.5A Arrange each of the following pairs of ions in order of increasing ionic radius: (a) Mg2ϩ and Al3ϩ; (b) O2Ϫ and S2Ϫ [Answer: (a) r(Al3ϩ) Ͻ r(Mg2ϩ); (b) r(O2Ϫ) Ͻ r(S2Ϫ)] Self-Test 2.5B Arrange each of the following pairs of ions in order of increasing ionic radius: (a) Ca2ϩ and Kϩ; (b) S2Ϫ and ClϪ Related Exercises 2.59, 2.60 Ionic radii generally increase down a group and decrease from left to right across a period Cations are smaller than their parent atoms, and anions are larger S S2Ϫ Cl FϪ ClϪ FIGURE 2.23 The relative sizes of some cations and anions compared with their parent atoms Note that cations (pink) are smaller than their parent atoms (gray), whereas anions (green) are larger c02QuantumMechanicsInActionAtoms.indd Page 54 5/25/12 7:19 PM user-F393 54 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms 2.10 Ionization Energy By referring to the minimum energy, we not have to worry about the kinetic energy of the electron: it is stationary Ionization can be achieved by using a higher energy, but then the electron would carry away the excess energy as kinetic energy We shall see in Chapter that the formation of a bond in an ionic compound depends on the removal of one or more electrons from one atom and their transfer to another atom The energy needed to remove electrons from atoms is therefore of central importance for understanding their chemical properties As remarked in Section 2.1, the ionization energy, I, is the minimum energy needed to remove an electron from an atom in the gas phase Specifically, X1g2 ¡ X ϩ 1g2 ϩ e Ϫ 1g2     I ϭ E1X ϩ Ϫ E1X2 (9)* For a single atom, the ionization energy is normally expressed in electronvolts (eV), the change in potential energy of an electron when it moves through a potential difference of volt (1 eV ϭ 1.602 ϫ 10Ϫ19 J) For a macroscopic sample, the ionization energy is expressed in kilojoules per mole of atoms (kJ∙molϪ1) The first ionization energy, I1, is the minimum energy needed to remove an electron from a neutral atom in the gas phase For example, for copper, Cu1g2 ¡ Cu ϩ 1g2 ϩ e Ϫ 1g2     energy required ϭ I1 17.73 eV, 746 kJؒmol Ϫ1 The second ionization energy, I2, of an element is the minimum energy needed to remove an electron from a singly charged gas-phase cation For copper, Cu ϩ 1g2 ¡ Cu2ϩ 1g2 ϩ e Ϫ 1g2     energy required ϭ I2 120.29 eV, 1958 kJؒmol Ϫ1 Because ionization energy is a measure of how difficult it is to remove an electron, elements with low ionization energies can be expected to form cations readily and to conduct electricity (which requires that some electrons be free to move) in their solid forms Elements with high ionization energies are unlikely to form cations and are unlikely to conduct electricity THINKING POINT Why is the second ionization energy of an atom always higher than its first ionization energy? As can be seen in FIG 2.24: • First ionization energies typically decrease down a group • First ionization energies generally increase across a period The decrease down a group can be explained by the finding that, in successive periods, the outermost electron occupies a shell that is farther from the nucleus and H 1310 2 13 14 15 16 17 Li 519 Be 900 B 799 C 1090 N 1400 O 1310 F 1680 Ne 2080 Na Mg Al Si P S Cl Ar 494 736 577 786 1011 1000 1255 1520 K 418 Ca 590 Ga 577 Ge 784 As 947 Se 941 Br 1140 Kr 1350 Rb 402 Sr 548 In 556 Sn 707 Sb 834 Te 870 I 1008 Xe 1170 Cs 376 Ba 502 Tl 590 Pb 716 Bi 703 Po 812 At 1037 Rn 1036 FIGURE 2.24 The first ionization energies of the main-group elements, in kilojoules per mole In general, low values are found at the lower left of the table and high values are found at the upper right 18 He 2370 c02QuantumMechanicsInActionAtoms.indd Page 55 6/14/12 6:20 PM user-F393 /Users/user-F393/Desktop 2.10 Ionization Energy 55 FIGURE 2.25 The periodic variation of the first ionization energies of the elements He Ne Ar Ionization energy H Kr Xe Rn Lanthanoids Actinoids Atomic number is therefore less tightly bound Therefore, it takes less energy to remove an electron from a cesium atom, for instance, than from a sodium atom With few exceptions, the first ionization energy rises from left to right across a period (FIG 2.25) This trend can be traced to the increase in effective nuclear charge across a period The small departures from this trend can be traced to repulsions between electrons, particularly electrons occupying the same orbital For example, the ionization energy of oxygen is slightly lower than that of nitrogen because in a nitrogen atom each p-orbital has one electron, but in oxygen the eighth electron is paired with an electron already occupying an orbital The repulsion between the two electrons in the same orbital raises their energy and makes one of them easier to remove from the atom than if the two electrons had been in different orbitals FIGURE 2.26 shows that the second ionization energy of an element is always higher than its first ionization energy It takes more energy to remove an electron from a positively charged ion than from a neutral atom For the Group elements, the second ionization energy is considerably larger than the first; in Group 2, however, the two ionization energies have similar values This difference makes sense, because the Group elements have an ns1 valence-shell electron configuration Although the removal of the first electron requires only a small amount of energy, the second electron must come from the noble-gas core The core electrons have lower principal quantum numbers and are much closer to the nucleus They are strongly attracted to it, and a lot of energy is needed to remove them Self-Test 2.6A Account for the slight decrease in first ionization energy between beryllium and boron [Answer: Boron loses an electron from a higher-energy subshell than beryllium does.] Self-Test 2.6B Account for the large decrease in third ionization energy between beryllium and boron ■ The low ionization energies of elements at the lower left of the periodic table account for their metallic character A block of metal consists of a collection of cations of the element surrounded by a sea of valence electrons that the atoms have 25 000 14 800 First Second Third Fourth 7300 3660 1760 4560 3070 2420 519 900 799 494 418 Be Na K Li B FIGURE 2.26 The successive ionization energies of a selection of main-group elements Note the great increase in energy required to remove an electron from an inner shell In each case, the blue outline denotes ionization from the valence shell c02QuantumMechanicsInActionAtoms.indd Page 56 5/25/12 7:19 PM user-F393 56 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms Metal block Cation Electron sea FIGURE 2.27 A block of metal consists of an array of cations (the spheres) surrounded by a sea of electrons The charge of the electron sea cancels the charges of the cations The electrons of the sea are mobile and can move past the cations quite easily and hence conduct an electric current ANIMATION FIGURE 2.27 lost (FIG 2.27) Only elements with low ionization energies—the members of the s-block, the d-block, the f-block, and the lower left of the p-block—can form metallic solids, because only they can lose electrons easily The elements at the upper right of the periodic table have high ionization energies; so they not readily lose electrons and are therefore not metals Note that our knowledge of electronic structure has helped us to understand a major feature of the periodic table—in this case, why the metals are found toward the lower left and the nonmetals are found toward the upper right The first ionization energy is highest for elements close to helium and is lowest for elements close to cesium Second ionization energies are higher than first ionization energies (of the same element) and very much higher if the electron is to be removed from a closed shell Metals are found toward the lower left of the periodic table because these elements have low ionization energies and can readily lose their electrons 2.11 Electron Affinity To predict some chemical properties, we need to know how the energy changes when an electron attaches to an atom The electron affinity, Eea, of an element is the energy released when an electron is added to a gas-phase atom A positive electron affinity means that energy is released when an electron attaches to an atom A negative electron affinity means that energy must be supplied to push an electron onto an atom This convention matches the everyday meaning of the term “affinity.” More formally, the electron affinity of an element X is defined as X1g2 ϩ e Ϫ 1g2 ¡ X Ϫ 1g2     Eea 1X2 ϭ E1X2 Ϫ E1X Ϫ (10)* where E(X) is the energy of a gas-phase X atom and E(XϪ) is the energy of the gas-phase anion For instance, the electron affinity of chlorine is the energy released in the process Cl1g2 ϩ e Ϫ 1g2 ¡ Cl Ϫ 1g2     energy released ϭ Eea 13.62 eV, 349 kJؒmol Ϫ1 In some books, you will see electron affinity defined with an opposite-sign convention Those values are actually the electron-gain enthalpies (Chapter 8) Because the electron has a lower energy when it occupies one of the atom’s orbitals, the difference E(Cl) Ϫ E(ClϪ) is positive and the electron affinity of chlorine is positive Like ionization energies, electron affinities are reported either in electronvolts for a single atom or in joules per mole of atoms FIGURE 2.28 shows the variation in electron affinity in the main groups of the periodic table It is much less periodic than variations in radius and ionization energy However, one broad trend is clearly visible With the exception of the noble gases: • Electron affinities are highest toward the right of the periodic table H ϩ73 FIGURE 2.28 The variation in electron affinity in kilojoules per mole of the main-group elements Where two values are given, the first refers to the formation of a singly charged anion and the second is the additional energy needed to produce a doubly charged anion The negative signs of the second values indicate that energy is required to add an electron to a singly charged anion The variation is less systematic than that for ionization energy, but high values tend to be found close to fluorine (though not for the noble gases) 13 14 15 Li ϩ60 Be Յ0 B ϩ27 C ϩ122 N Ϫ7 Na ϩ53 Mg Յ0 Al ϩ43 Si ϩ134 P ϩ72 K ϩ48 Ca ϩ2 Ga ϩ29 Ge ϩ116 As ϩ78 Rb ϩ47 Sr ϩ5 In ϩ29 Sn ϩ116 I Te Sb ϩ103 ϩ190 ϩ295 Xe Ͻ0 Cs ϩ46 Ba ϩ14 Tl ϩ19 Pb ϩ35 At ϩ270 Rn Ͻ0 Bi ϩ91 16 17 O F ϩ141 Ϫ844 ϩ328 S Cl ϩ200, Ϫ532 ϩ349 Br Se ϩ195 ϩ325 18 He Ͻ0 Po ϩ174 Ne Ͻ0 Ar Ͻ0 Kr Ͻ0 c02QuantumMechanicsInActionAtoms.indd Page 57 5/25/12 7:19 PM user-F393 /Users/user-F393/Desktop 2.11 Electron Affinity 57 This trend is particularly true in the upper right, close to oxygen, sulfur, and the halogens In these atoms, the incoming electron occupies a p-orbital close to a nucleus with a high effective charge and can experience its attraction quite strongly The noble gases have negative electron affinities because any electron added to them must occupy an orbital outside a closed shell and far from the nucleus; this process requires energy, and so the electron affinity is negative Once an electron has entered the single vacancy in the valence shell of a Group 17 atom, the shell is complete and any additional electron would have to begin a new shell In that shell, it not only would be farther from the nucleus but would also feel the repulsion of the negative charge already present As a result, the second electron affinity of fluorine is strongly negative, meaning that a lot of energy has to be expended to form F2Ϫ from FϪ Ionic compounds of the halogens are therefore built from singly charged ions such as FϪ and never from doubly charged ions such as F2Ϫ A Group 16 atom, such as O or S, has two vacancies in its valence-shell p-orbitals and can accommodate two additional electrons The first electron affinity is positive because energy is released when an electron attaches to O or S However, attachment of the second electron requires energy because of the repulsion by the negative charge already present in OϪ or SϪ Unlike that of a halide ion, however, the valence shell of the OϪ anion has only seven electrons and thus can accommodate an additional electron Therefore, we expect that less energy will be needed to make O2Ϫ from OϪ than to make F2Ϫ from FϪ, where no such vacancy exists In fact, 141 kJ·molϪ1 is released when the first electron adds to the neutral atom to form OϪ, but 844 kJ·molϪ1 must be supplied to add a second electron to form O2Ϫ; so the total energy required to make O2Ϫ from O is ϩ703 kJ·molϪ1 As we shall see in Chapter 3, this energy can be achieved in chemical reactions, and O2Ϫ ions are common in metal oxides EXAMPLE 2.4 Predicting trends in electron affinity Organic chemists need to think about the distribution of electrons in molecules, because electron-rich regions might prove to be centers of attack for reagents One guide (not the only one) to where electrons are likely to accumulate is the electron affinity of the element The electron affinity of carbon is greater than that of nitrogen; indeed, the latter is negative Suggest a reason for this observation SOLVE More energy is expected to be released when an electron enters the N atom, because an N atom is smaller than a C atom and its nucleus is more highly charged: the effective nuclear charges for the outermost electrons of the neutral atoms are 3.8 for N and 3.1 for C However, the opposite is observed, and so the effective nuclear charges experienced by the valence electrons in the anions must also be considered (FIG 2.29) When CϪ forms from C, the additional electron occupies an empty 2p-orbital (see 6) The incoming electron is well separated from the other p-electrons, and so it experiences an effective nuclear charge close to 3.1 When NϪ forms from N, the additional electron must occupy a 2p-orbital that is already half full (see 7) The effective nuclear charge experienced by this electron is therefore much less than 3.8; so energy is required to form NϪ, and the electron affinity of nitrogen is lower than that of carbon Self-Test 2.7A Account for the large decrease in electron affinity between lithium and beryllium [Answer: The additional electron enters a 2s-orbital in Li but a 2p-orbital in Be, and a 2s-electron is more tightly bound than a 2p-electron.] Self-Test 2.7B Account for the large decrease in electron affinity between fluorine and neon Related Exercises 2.67, 2.68 Elements with the highest electron affinities are those in Groups 16 and 17 Before After Before After Energy PLAN When a periodic trend is different from what is expected, you should examine the electron configurations of all the species to look for clues to the observed behavior (a) Carbon (b) Nitrogen FIGURE 2.29 The energy changes that take place when an electron is added to a carbon atom and a nitrogen atom (a) A carbon atom can accommodate an additional electron in an empty p-orbital (b) When an electron is added to a nitrogen atom, it must pair with an electron in a p-orbital The incoming electron experiences so much repulsion from those already present in the nitrogen atom that the electron affinity of nitrogen is less than that of carbon and is in fact negative c02QuantumMechanicsInActionAtoms.indd Page 58 6/21/12 4:06 PM user-F393 /Users/user-F393/Desktop Chapter Quantum Mechanics in Action: Atoms 58 2.12 The Inert-Pair Effect FIGURE 2.30 When tin(II) oxide is heated in air, it becomes incandescent as it reacts to form tin(IV) oxide Even without being heated, it smolders and can ignite Zn Al Si P S Ga Ge As Se In+ Sn2+ Sb3+ Cd In3+ Sn4+ Sb5+ + Pb2+ Bi3+ Tl3+ Pb4+ Bi5+ Hg Tl 18 14 15 Li Be B C N Na Mg Al Si K Ca Ga Ge As 16 The inert-pair effect is the tendency to form ions two units lower in charge than expected from the group number; it is most pronounced for heavy elements in the p-block 2.13 Diagonal Relationships FIGURE 2.31 The typical ions formed by the heavy elements in Groups 13 through 15 show the influence of the inert pair—the tendency to form compounds in which the oxidation numbers differ by 13 Although both aluminum and indium are in Group 13, aluminum forms Al3ϩ ions, whereas indium forms both In3ϩ and Inϩ ions The tendency to form ions two units lower in charge than expected from the group number is called the inert-pair effect Another example of the inert-pair effect is found in Group 14: tin forms tin(IV) oxide when heated in air, but the heavier lead atom loses only its two p-electrons and forms lead(II) oxide Tin(II) oxide can be prepared, but it is readily oxidized to tin(IV) oxide (FIG 2.30) Lead exhibits the inert-pair effect more strongly than tin The inert-pair effect is due in part to the relative energies of the valence p- and s-electrons In the later periods of the periodic table, valence s-electrons are very low in energy because of their good penetration and the low shielding ability of the d-electrons The valence s-electrons may therefore remain attached to the atom during ion formation The inert-pair effect is most pronounced among the heaviest members of a group, where the difference in energy between s- and p-electrons is greatest (FIG 2.31) Even so, the pair of s-electrons can be removed from the atom under sufficiently vigorous conditions An inert pair would be better called a “lazy pair” of electrons A diagonal relationship is a similarity in properties between diagonal neighbors in the main groups of the periodic table (FIG 2.32) A part of the reason for this similarity can be seen in Figs 2.20 and 2.24 by concentrating on the colors that show the general trends in atomic radius and ionization energy The colored bands of similar values lie in diagonal stripes across the table Because these characteristics affect the chemical properties of an element, it is not surprising to find that the elements within a diagonal band show similar chemical properties (FIG 2.33) Diagonal relationships are helpful for making predictions about the properties of elements and their compounds The diagonal band of metalloids dividing the metals from the nonmetals is one example of a diagonal relationship (Fundamentals, Section B) So is the chemical similarity of lithium and magnesium and of beryllium and aluminum For example, both lithium and magnesium react directly with nitrogen to form nitrides Like aluminum, beryllium reacts with both acids and bases We shall see many examples of this diagonal similarity when we look at the main-group elements in detail in Chapter 16 Diagonally related pairs of elements often show similar chemical properties 17 P FIGURE 2.32 The pairs of elements represented by similarly colored boxes show a strong diagonal relationship to each other 2.14 The General Properties of the Elements We are now at the point where we can begin to predict, in at least a general way, the properties of elements For example, an s-block element has a low ionization energy, which means that its outermost electrons can easily be lost An s-block element is therefore likely to be a reactive metal with all the characteristics that the name “metal” implies (TABLE 2.3, FIG 2.34) Because ionization energies are lowest at the bottom of each group and the elements there lose their valence electrons most easily, cesium and barium react most vigorously of all s-block elements and have to be stored out of contact with air and water Elements on the left of the p-block, especially the heavier elements, have ionization energies that are low enough for these elements to have some of the metallic properties of the members of the s-block However, the ionization energies of the p-block metals are quite high, and they are less reactive than those in the s-block (FIG 2.35) Elements at the right of the p-block (with the exception of the noble gases) have characteristically high electron affinities: they tend to gain electrons to complete ... Illustration Coordinator: Bill Page Illustrations: Peter Atkins and Leroy Laverman with © 201 3, 201 0, 200 5, 2002 by P W Atkins, L L Jones and L E Laverman All rights reserved Network Graphics Production... Orientation, Matter and Energy, Elements and Atoms, Compounds, The Nomenclature of Compounds, Moles and Molar Masses, Determination of Chemical Formulas, Mixtures and Solutions, Chemical Equations, Aqueous... fully to this new edition Yours sincerely, Peter Atkins, Loretta Jones, and Leroy Laverman xii FMTOC.indd Page xiii 10/18/12 8:07 PM user-F393 /Users/user-F393/Desktop Preface Chemical Principles