AP CHEMISTRY EXAM Fall review Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Energy and Chemistry ENERGY is the capacity to do work or transfer heat. HEAT is the form of energy that flows between 2 samples because of their difference in temperature. Other forms of energy — • light • electrical • kinetic and potential Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Kinetic and Potential Energy Potential energy — energy a body has because of its position. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Kinetic and Potential Energy Kinetic energy — energy of motion. • Translation • Rotation • Vibration Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics • Thermodynamics is the science of heat (energy) transfer. Heat energy is associated with molecular motions. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Energy and Chemistry All of thermodynamics depends on the law of THE CONSERVATION OF ENERGY. • The total energy of a system is constant. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved UNITS OF ENERGY 1 calorie = heat to raise temp. of 1.00 g of H2O by 1.0 oC. 1000 cal = 1 kilocalorie = 1 kcal But we use the unit called the JOULE 1 cal = 4.184 joules Copyright (c) 1999 by Harcourt Brace & Company All rights reserved James Joule 1818-1889 Specific Heat Capacity The heat “lost” or “gained” is related to a) sample mass b) change in T and c) specific heat capacity by Specific heat capacity = heat lost or gained by substance (J) (mass, g)(T change, K) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Specific Heat Capacity Substance H2O Al glass Spec. Heat (J/g•K) 4.184 0.902 0.84 Aluminum Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Specific Heat Capacity If 25.0 g of Al cool from 310 oC to 37 oC, how many joules of heat energy are lost by the Al? Specific heat capacity = heat lost or gained by substance (J) (mass, g)(T change, K) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Specific Heat Capacity If 25.0 g of Al cool from 310 oC to 37 oC, how many joules of heat energy are lost by the Al? heat gain or loss = q = (SH)(mass)(DT) q = (0.902 J/g•K)(25.0 g)(37 - 310)K q = - 6160 J The negative sign on q signals heat “lost by” or transferred out of Al. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Heat Transfer and Changes of State Changes of state involve energy Ice -----> Water 333 J/g (fusion) An ENDOTHERMIC process. + energy Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Heat and Changes of State • 1 g of ethanol requires 850 J to evaporate at 25 oC. • To drop air temp. from 55 oC to 25 oC in a car requires air to give up 3.6 kJ. • How much ethanol must be evaporated to do this? Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Heat and Changes of State 3.6 x 103 J (1 g/850 J) = 4.2 g of ethanol Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Heat and Changes of State What quantity of heat is required to melt 500. g of ice and heat the water to steam at 100 oC? Specific heat of water = 4.2 J/g•K Heat of fusion of ice = 333 J/g Heat of vaporization = 2260 J/g +333 J/g Copyright (c) 1999 by Harcourt Brace & Company All rights reserved +2260 J/g Heating/Cooling Curve for Water See Figure 6.9 3 Evaporate water Heat water 1 2 Melt ice Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 4 Heat and Changes of State What quantity of heat is required to melt 500. g of ice and heat the water to steam at 100 oC? 1. To melt ice q = (500. g)(333 J/g) = 1.67 x 105 J 2. To raise water from 0 oC to 100 oC q = (500. g)(4.2 J/g•K)(100 - 0)K = 2.1 x 105 J 3. To evaporate water at 100 oC q = (500. g)(2260 J/g) = 1.13 x 106 J 4. Total heat energy = 1.51 x 106 J = 1510 kJ Copyright (c) 1999 by Harcourt Brace & Company All rights reserved ENTHALPY DH = Hfinal - Hinitial If Hfinal > Hinitial then DH is positive Process is ENDOTHERMIC If Hfinal < Hinitial then DH is negative Process is EXOTHERMIC Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Endo- and Exothermic Surroundings System heat Surroundings System heat qsystem > 0 qsystem < 0 T(system) goes up T(system) goes down ENDOTHERMIC EXOTHERMIC Copyright (c) 1999 by Harcourt Brace & Company All rights reserved USING ENTHALPY Calc. DH for S(s) + 3/2 O2(g) --> SO3(g) knowing that S(s) + O2(g) --> SO2(g) DH1 = -320.5 kJ SO2(g) + 1/2 O2(g) --> SO3(g) DH2 = -75.2 kJ The two equations add to give the desired equation (at top), so DHnet = DH1 + DH2 = -395.7 kJ Copyright (c) 1999 by Harcourt Brace & Company All rights reserved energy S solid direct path + 3/2 O2 DH = -395.7 kJ SO3 gas +O2 DH 1 = -320.5 kJ SO2 gas + 1/2 O2 DH 2 = -75.2 kJ DH along one path = DH along another path Copyright (c) 1999 by Harcourt Brace & Company All rights reserved DH along one path = DH along another path • This equation is valid because DH is a STATE FUNCTION • These depend only on the state of the system and not how it got there. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Standard Enthalpy Values Standard enthalpy: DHo Measured under standard conditions P = 1 bar (1 atmosphere) Concentration = 1 mol/L T = usually 25 oC with all species in standard states e.g., C = graphite and O2 = gas DHof = 0 for elements in their standard states. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Using Standard Enthalpy Values Calculate ²H of reaction? In general, when ALL enthalpies of formation are known, DHorxn = DHof (products) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved - DHof (reactants) Electromagnetic Radiation • Most subatomic particles behave as PARTICLES and obey the physics of waves. • Wavelength, • Node • Amplitude Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electromagnetic Radiation wavelength Visible light Amplitude wavelength Node Ultraviolet radiation Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electromagnetic Radiation • Waves have a frequency • Greek letter “nu”, , = frequency. Units are “cycles per sec” • All radiation: • = c • c = velocity of light = 3.00 x 108 m/sec • Note that long wavelength --> small frequency • Short wavelength --> high frequency Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electromagnetic Radiation Red light has = 700 nm. Calculate the frequency. -9 1 x 10 m -7 700 nm • = 7.00 x 10 m 1 nm 8 Freq = 3.00 x 10 m/s 7.00 x 10 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved -7 m 4.29 x 1014 sec -1 Quantization of Energy Max Planck (1858-1947) Energy of radiation is proportional to frequency. E = h• h = Planck’s constant = 6.6262 x 10-34 J•s Suggests light is a particle (PHOTON) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Quantization of Energy E = h• Light with large (small ) has a small E. Light with a short (large ) has a large E. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Energy of Radiation PROBLEM: Calculate the energy of 1.00 mol of photons of red light. = 700. nm = 4.29 x 1014 sec-1 E = h• = (6.63 x 10-34 J•s)(4.29 x 1014 sec-1) = 2.85 x 10-19 J per photon Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Atomic Line Spectra and Niels Bohr Niels Bohr (1885-1962) A great accomplishment. Rec’d Nobel Prize, 1922 Problems with theory — • only successful for H. • introduced quantum idea artificially. • So, we go on to QUANTUM or WAVE MECHANICS Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Quantum or Wave Mechanics de Broglie (1924) proposed that all moving objects have wave properties. For light: E = mc2 L. de Broglie (1892-1987) E = h = hc / Therefore, mc = h / and for particles Copyright © 1999 by Harcourt Brace & Company All rights reserved. Requests for permission to make copies of any part of the work should be mailed to: Permissions Department, Harcourt Brace & Company, 6277 Sea Harbor Drive, Orlando, Florida 32887-6777 (mass)(velocity) = h / Quantum or Wave Mechanics E. Schrodinger 1887-1961 Solution to wave equation gives set of mathematical expressions called WAVE FUNCTIONS, Each describes an allowed energy state of an eQuantization introduced naturally. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved WAVE FUNCTIONS, • Each corresponds to an ORBITAL — the region of space within which an electron is found. • does NOT describe the exact location of the electron. • 2 is proportional to the probability of finding an e- at a given point. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Uncertainty Principle W. Heisenberg 1901-1976 Solved problem of defining nature of electrons in atoms. Cannot define position and momentum (= m•v) of an electron simultaneously. We define e- energy exactly but accept limitation that we do not know exact position. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved QUANTUM NUMBERS Electrons are arranged in shells and subshells. n --> shell (energy level) l --> subshell (orbital shape) ml --> designates an orbital within a subshell (orintation on a coordinate system) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved s Orbitals n = 1, l = 0 In first shell, there is 1 orbital. All s orbitals are spherical in shape. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Typical p orbital p Orbitals When n = 2, then l = 0 and planar 1 node in n = 2 shell there are 2 types of orbitals — 2 subshells For l = 0 ml = 0 this is a s subshell For l = 1 ml = -1, 0, +1 this is a p subshell with 3 orbitals each oriented on an axis. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved d Orbitals When n = 3, l = 0, 1, 2 there are 3 subshells in the shell. For l = 0, ml = 0 ---> s subshell with single orbital For l = 1, ml = -1, 0, +1 ---> p subshell with 3 orbitals For l = 2, ml = -2, -1, 0, +1, +2 ---> d subshell with 5 orbitals Copyright (c) 1999 by Harcourt Brace & Company All rights reserved d Orbitals typical d orbital planar node planar node Copyright (c) 1999 by Harcourt Brace & Company All rights reserved f Orbitals When n = 4, l = 0, 1, 2, 3 so there are 4 subshells in the shell. For l = 0, ml = 0 ---> s subshell with single orbital For l = 1, ml = -1, 0, +1 ---> p subshell with 3 orbitals For l = 2, ml = -2, -1, 0, +1, +2 ---> d subshell with 5 orbitals For l = 3, ml = -3, -2, -1, 0, +1, +2, +3 ---> f subshell with 7 orbitals Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Arrangement of Electrons in Atoms Each orbital can be assigned no more than 2 electrons! This is tied to the existence of a 4th quantum number, the electron spin quantum number, ms. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electron Spin Quantum Number Diamagnetic: NOT attracted to a magnetic field Paramagnetic: substance is attracted to a magnetic field. Substance has unpaired electrons. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Pauli Exclusion Principle No two electrons in the same atom can have the same set of 4 quantum numbers. That is, each electron has a unique address. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electron Filling Order Figure 8.7 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Writing Atomic Electron Configurations Two ways of writing econfigs. One is called spectroscopic notation. SPECTROSCOPIC NOTATION for H, atomic number = 1 1 1s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved value of n no. of electrons value of l Writing Atomic Electron Configurations ORBITAL BOX NOTATION for He, atomic number = 2 Arrows 2 depict electron spin 1s 1s Two ways of writing configs. Other is called the orbital box notation. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Lithium Group 1A Atomic number = 3 1s22s1 ---> 3 total electrons Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Boron 3p 3s 2p 2s 1s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Group 3A Atomic number = 5 1s2 2s2 2p1 ---> 5 total electrons Carbon 3p 3s 2p 2s 1s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Group 4A Atomic number = 6 1s2 2s2 2p2 ---> 6 total electrons HUND’S RULE. When placing electrons in orbitals of the same energy, place them singly as long as possible. Oxygen 3p 3s 2p 2s 1s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Group 6A Atomic number = 8 1s2 2s2 2p4 ---> 8 total electrons Neon 3p 3s 2p 2s 1s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Group 8A Atomic number = 10 1s2 2s2 2p6 ---> 10 total electrons We have reached the end of the 2nd period, and the 2nd shell is full! Sodium Group 1A Atomic number = 11 1s2 2s2 2p6 3s1 or “neon core” + 3s1 [Ne] 3s1 (uses rare gas notation) All Group 1A elements have [core]ns1 configurations. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Relationship of Electron Configuration and Region of the Periodic Table • Gray = s block • Orange = p block • Green = d block • Violet = f block Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Transition Element Configurations 3d orbitals used for Sc - Zn (Table 8.4) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Lanthanide Element Configurations 4f orbitals used for Ce - Lu and 5f for Th - Lr (Table 8.2) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ion Configurations To form cations from elements remove 1 or more e- from subshell of highest n [or highest (n + l)]. P [Ne] 3s2 3p3 - 3e- ---> P3+ [Ne] 3s2 3p0 3p 3p 3s 3s 2p 2p 2s 2s 1s 1s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved General Periodic Trends • Atomic and ionic size • Ionization energy • Electron affinity Higher Z*. Electrons held more tightly. Larger orbitals. Electrons held less tightly. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Atomic Size SIZE • Size goes UP going down a group. • Electrons are added further from the nucleus, there is less attraction. • Size goes DOWN going across a period. • Due to the increase in Z*. Each added electron feels a greater and greater + charge. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ion Sizes + Li,152 pm 3e and 3p Li +, 60 pm 2e and 3 p Forming a cation. • CATIONS are SMALLER than the atoms from which they come. • The electron/proton attraction has gone UP and so size DECREASES. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ion Sizes F,64 pm 9e and 9p F- , 136 pm 10 e and 9 p Forming an anion. • ANIONS are LARGER than the atoms from which they come. • The electron-proton attraction has gone DOWN so size INCREASES. • Trends in ion sizes are the same as atom sizes. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Redox Reactions Why do metals lose electrons in their reactions? Why does Mg form Mg2+ ions and not Mg3+? Why do nonmetals take on electrons? Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ionization Energy See Screen 8.12 IE = energy required to remove an electron from an atom in the gas phase. Mg (g) + 738 kJ ---> Mg+ (g) + e- Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ionization Energy See Screen 8.12 IE = energy required to remove an electron from an atom in the gas phase. Mg (g) + 738 kJ ---> Mg+ (g) + eMg+ (g) + 1451 kJ ---> Mg2+ (g) + e- Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ionization Energy See Screen 8.12 IE = energy required to remove an electron from an atom in the gas phase. Mg (g) + 738 kJ ---> Mg+ (g) + eMg+ (g) + 1451 kJ ---> Mg2+ (g) + e- Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ionization Energy See Screen 8.12 IE = energy required to remove an electron from an atom in the gas phase. Mg (g) + 738 kJ ---> Mg+ (g) + eMg+ (g) + 1451 kJ ---> Mg2+ (g) + e- Mg+ has 12 protons and only 11 electrons. + > Mg. Therefore, IE for Mg Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ionization Energy See Screen 8.12 Mg (g) + 735 kJ ---> Mg+ (g) + eMg+ (g) + 1451 kJ ---> Mg2+ (g) + eMg2+ (g) + 7733 kJ ---> Mg3+ (g) + e- Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ionization Energy IE = energy required to remove an electron from an atom in the gas phase. Mg (g) + 735 kJ ---> Mg+ (g) + e- Mg+ (g) + 1451 kJ ---> Mg2+ (g) + eMg2+ (g) + 7733 kJ ---> Mg3+ (g) + e- Energy cost is very high to dip into a shell of lower n. This is why ox. no. = Group no. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Trends in Ionization Energy 1st Ionization energy (kJ/mol) 2500 He Ne 2000 Ar 1500 Kr 1000 500 0 1 H 3 Li 5 7 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 9 11 Na 13 15 17 19 K 21 23 25 27 29 31 Atomic Number 33 35 Trends in Ionization Energy • IE increases across a period because Z* increases. • Metals lose electrons more easily than nonmetals. • Metals are good reducing agents. • Nonmetals do not lose electrons. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Trends in Ionization Energy • IE decreases down a group • Because size increases. • Reducing ability generally increases down the periodic table. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electron Affinity A few elements GAIN electrons to form anions. Electron affinity is the energy involved when an anion loses an electron. A-(g) ---> A(g) + eE.A. = DE Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Trends in Electron Affinity • Affinity for electron increases across a period (EA becomes more positive). • Affinity decreases down a group (EA becomes less positive). Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Atom EA F +328 kJ Cl +349 kJ Br +325 kJ I +295 kJ Trends in Electron Affinity F Cl Br 35 0 30 0 S Si 20 0 Se 15 0 S4 10 0 Ge P S3 Period 50 S2 S1 0 K 1 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2 3 4 5 Group 6 7 Elec tron affinity (kJ/m ol) C H 25 0 O Forms of Chemical Bonds • There are 2 extreme forms of connecting or bonding atoms: • Ionic—complete transfer of electrons from one atom to another • Covalent—electrons shared between atoms • Most bonds are somewhere in between. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electron transfer from an element of low IE (metal) to an element of high EA (nonmetal) 2 Na(s) + Cl2(g) ---> 2 Na+ + 2 ClUsually between: Groups 1A , 2A & transition metals and Nonmetals (O and halogens). Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Ionic Bonds Covalent Bonding Covalent bonds form by sharing VALENCE ELECTRONS, those at the outer edge of the atom. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Valence Electrons Electrons are divided between core and valence electrons. Na 1s2 2s2 2p6 3s1 Core = [Ne] and valence = 3s1 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 1A Valence Electrons 2A 3A 4A 5A 6A Number of valence electrons is equal to Group number. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 8A 7A Covalent Bonding The bond arises from the mutual attraction of 2 nuclei for the same electrons. Bond is a balance of attractive and repulsive forces. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electron Distribution in Molecules G. N. Lewis 1875 - 1946 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved • Electron distribution is shown by Lewis electron dot structures • Electrons are distributed as shared or BOND PAIRS and unshared or LONE PAIRS. Bond and Lone Pairs • Electrons are distributed as shared or BOND PAIRS and unshared or LONE PAIRS. •• H Cl • • •• shared or bond pair Copyright (c) 1999 by Harcourt Brace & Company All rights reserved lone pair (LP) Bond Formation A bond can result from a “head-tohead” overlap of atomic orbitals on neighboring atoms. •• H + Cl •• •• • • H Overlap of H (1s) and Cl (2p) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Cl •• • • Bond Formation A bond can result from a “head-to-head” overlap of atomic orbitals on neighboring atoms. •• H + Cl •• •• • • H Cl • • •• Overlap of H (1s) and Cl (2p) This overlap puts bonding electrons in a MOLECULAR ORBITAL along the line between the two atoms and forms a SIGMA BOND (). Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Rules of the Game •No. of valence electrons of an atom = Group number •For Groups 1A-4A, no. of bond pairs expected = group number • For Groups 5A-7A, BP’s = 8 - Grp. No. •Except for H (and atoms of 3rd and higher periods), BP’s + LP’s = 4 (8 electrons) This is the OCTET Copyright (c) 1999 by Harcourt Brace & Company All rights reserved RULE Building a Dot Structure Ammonia, NH3 1. Decide on the central atom; never H. Central atom has lowest EA. Therefore, N is central 2. Count valence electrons H = 1 and N = 5 Total = (3 x 1) + 5 = 8 electrons / 4 pairs Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Building a Dot Structure 3. Form a sigma bond between the central atom and surH N rounding atoms. H H 4. Remaining e- form LONE PAIRS to complete octet as needed. 3 BOND PAIRS and 1 LONE PAIR. N has a share in 4 pairs (8 e-), while H shares 1 pair. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Carbon Dioxide, CO2 1. Central atom = C 2. Valence electrons = 16 (8 pair) 3. Form sigma bonds, leaving 6 pair. 4. Place lone pairs on outer atoms. •• •• • • O •• Copyright (c) 1999 by Harcourt Brace & Company All rights reserved C O •• • • Carbon Dioxide, CO2 4. Place lone pairs on outer atoms. 5. So C has an octet, form DOUBLE BONDS between C and O. •• •• • • O •• C O • • •• The second bonding pair forms a pi (p) bond. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved • • O •• C O •• • • Double and even triple bonds are commonly observed for C, N, P, O, and S H2CO SO3 • • C2F4 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved O •• C O •• • • Sulfur Dioxide, SO2 OR bring in right pair bring in left pair •• •• • • O •• S •• O • • •• This leads to the following structures. •• • • O •• S Copyright (c) 1999 by Harcourt Brace & Company All rights reserved •• • • O •• •• • • •• O •• S • • O •• Sulfur Dioxide, SO2 18 electrons can be distributed in two ways with the following structures. •• • • •• • • O S O •• •• •• •• • • •• • • O S O •• These equivalent structures are called RESONANCE STRUCTURES. The true electronic structure is a HYBRID of the two. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Violations of the Octet Rule Usually occurs with B and elements of higher periods. BF3 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved SF4 MOLECULAR GEOMETRY VSEPR Valence Shell Electron Pair Repulsion theory. Molecule Most important factor adopts the in determining geometry shape that minimizes the is relative repulsion electron pair between electron pairs. repulsions. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved No. of e- Pairs Around Central Atom 2 Example F—Be—F Geometry linear 180 F 3 F planar trigonal B F 120 H 4 C H Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 109 tetrahedral H H No. of e- Pairs Around Central Atom 2 Example F—Be—F Geometry linear 180 F 3 F planar trigonal B F 120 H 4 C H Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 109 tetrahedral H H No. of e- Pairs Around Central Atom 2 Example F—Be—F Geometry linear 180 F 3 F planar trigonal B F 120 H 4 C H Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 109 tetrahedral H H Structure Determination by VSEPR •• H N H Ammonia, NH3 H 1. Draw electron dot structure 2. Count BP’s and LP’s = 4 3. The 4 electron pairs are at the corners of a tetrahedron. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Structure Determination by VSEPR Ammonia, NH3 •• H N H ELECTRON PAIR GEOMETRY is tetrahedral. H MOLECULAR GEOMETRY (position of the atoms) is PYRAMIDAL. lone pair of electrons in tetrahedral position N H H H Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Structure Determination by VSEPR Formaldehyde, CH2O • • O • • The electron pair geometry is PLANAR TRIGONAL C H H The molecular geometry is also planar trigonal. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Structure Determination by VSEPR Methanol, CH3OH 1. Draw electron dot structure Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Violations of the Octet Rule Consider boron trifluoride, BF3 The B atom is surrounded by only 3 electron pairs. Bond angles are 120o •• • • • • F •• • • F •• B • • Geometry described as planar trigonal Copyright (c) 1999 by Harcourt Brace & Company All rights reserved • • F •• Compounds with 5 or More Pairs Around the Central Atom 90 F F P Trigonal bipyramid F 120 5 electron pairs F F 90 6 electron pairs F F S F Copyright (c) 1999 by Harcourt Brace & Company All rights reserved F Octahedron F F 90 Bond Order the number of bonds between a pair triple, BO = 3 of atoms. H H H C C 1 and 2 p C single double, BO = 2 BO = 1 1 and 1 p 1 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved N Bond Order Bond order is proportional to two important bond properties: (a) bond strength (b) bond length 110 pm 745 kJ 414 kJ Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 123 pm Bond Length Bond length is the distance between the nuclei of two bonded atoms. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Bond Length Bond length depends on size of bonded atoms and bond order. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Bond Strength The energy needed to break a bond. • BOND STRENGTH (kJ/mol) H—H 436 C—C 346 C=C 602 CC 835 The GREATER the number of bonds (bond order) the HIGHER the bond strength, the SHORTER the bond. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Using Bond Energies Estimate the energy of the reaction H—H + Cl—Cl ----> 2 H—Cl Net energy = DHrxn = = energy required to break bonds - energy given off when bonds are made Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Using Bond Energies Estimate the energy of the reaction H—H + Cl—Cl ----> 2 H—Cl Net energy = DHrxn = = energy required to break bonds - energy evolved when bonds are made H—H = 436 kJ/mol Cl—Cl = 242 kJ/mol H—Cl = 432 kJ/mol Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Using Bond Energies Estimate the energy of the reaction H—H + Cl—Cl ----> 2 H—Cl H—H = 436 kJ/mol Cl—Cl = 242 kJ/mol H—Cl = 432 kJ/mol Sum of H-H + Cl-Cl bond energies = 436 kJ + 242 kJ = +678 kJ 2 mol H-Cl bond energies = +864 kJ Net = DH = +678 kJ - 864 kJ = -186 kJ Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Bond Polarity + H - •• Cl •• •• Copyright (c) 1999 by Harcourt Brace & Company All rights reserved HCl is POLAR because it has a positive end and a negative end. Polarity arises because Cl has a greater share in bonding electrons than does H. + H - •• Cl •• Bond Polarity •• Due to bond polarity, the H—Cl bond energy is GREATER than expected for a “pure” covalent bond. BOND ENERGY “pure” bond 339 kJ/mol calculated real bond 432 kJ/mol measured Difference = 92 kJ, proportional to the difference in ELECTRONEGATIVITY, . Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Electronegativity, is a measure of the ability of an atom in a molecule to attract electrons to itself. • F has maximum . • Atom with lowest is the center atom in most molecules. • Values of in bonded atoms determine Linus Pauling BOND POLARITY. 1901-1994 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Bond Polarity Which bond is more polar (or DIPOLAR)? O—H O—F 3.5 - 2.1 3.5 - 4.0 D 1.4 0.5 OH is more polar than OF O—H - + O—F + - and polarity is “reversed.” Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Molecular Polarity Molecules—such as HCl and H2O— can be POLAR (or dipolar). They have a DIPOLE MOMENT. The polar HCl molecule will turn to align with an electric field. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Molecular Polarity Molecules—such as HCl and H2O— can be POLAR (or dipolar). They have a DIPOLE MOMENT. The polar HCl molecule will turn to align with an electric field. POSITIVE Copyright (c) 1999 by Harcourt Brace & Company All rights reserved H—Cl NEGATIVE Molecular Polarity Molecules will be polar if a) bonds are polar AND b) the molecule is NOT “symmetric” Symmetric molecules Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Molecular Polarity, H 2O •• O •• H H polar Copyright (c) 1999 by Harcourt Brace & Company All rights reserved O H H + Carbon Dioxide • • O •• C Copyright (c) 1999 by Harcourt Brace & Company All rights reserved O •• • • • CO2 is NOT polar even though the CO bonds are polar. Two Theories of Bonding • MOLECULAR ORBITAL THEORY — Robert Mullikan (1896-1986) • valence electrons are delocalized • valence electrons are in molecular orbitals which spread over entire molecule. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Two Theories of Bonding • VALENCE BOND THEORY — Linus Pauling • valence electrons are localized between atoms (or are lone pairs). • half-filled atomic orbitals overlap to form bonds. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Sigma Bond Formation by Orbital Overlap H H • + • • • sigma bond ( ) Two p orbitals overlap Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Two s orbitals overlap Bonding in BF3 ORBITAL HYBRIDIZATION mix available orbitals to form a new set of orbitals — HYBRID ORBITALS — that give the maximum overlap in the correct geometry. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Bonding in BF3 2s hydridize orbs. 2p rearrange electrons 2 three sp hybrid orbitals Copyright (c) 1999 by Harcourt Brace & Company All rights reserved unused p orbital Bonding in a Tetrahedron — Formation of Hybrid Atomic Orbitals 4 C atom orbitals hybridize to form four equivalent sp3 hybrid atomic orbitals. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Orbital Hybridization BONDS SHAPE HYBRID REMAIN linear 3 trigonal sp2 planar 1p 4 tetrahedral sp3 none Copyright (c) 1999 by Harcourt Brace & Company All rights reserved sp 2 p’s 2 Multiple Bonds Consider ethylene, C2H4 H H 120 o C H Copyright (c) 1999 by Harcourt Brace & Company All rights reserved sp C H 2 p Bonding in C2H4 The unused p orbital on each C contains an electron. The two p orbitals overlap to form the p bond. 2s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2p 3 sp 2 hybrid orbitals p orb. for š bond Multiple Bonding in C2H4 Note that sp2 bonds give trigonal planar shape at each C. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Consequences of Multiple Bonding Restricted rotation around C=C bond. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Importance of carbon Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved The addition of various functional groups to ethylene results in ADDITION polymers. H H X Y \ / | | C==C + XY H--C---C--H / \ | | H H H H Copyright (c) 1999 by Harcourt Brace & Company All rights reserved ADDITION polymers: Polyvinyl chloride Vinyl acetate H Cl Teflon \ / Polypropylene C==C Polymethyl / \ pentane H H Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved HCl is removed (in a CONDENSATION reaction) Water is removed Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Amides This is the carbon portion of an amine (R-NH3) N O || The C-N (amide group) is important in natural polymers such as proteins, and synthetic polymers like nylon. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved IDEAL GAS LAW PV=nRT Brings together gas properties. Can be derived from experiment and theory. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Boyle’s Law If n and T are constant, then PV = (nRT) = k This means, for example, that P goes up as V goes down. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Robert Boyle (1627-1691). Son of Early of Cork, Ireland. Charles’s Law If n and P are constant, then V = (nR/P)T = kT V and T are directly related. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Jacques Charles (17461823). Isolated boron and studied gases. Balloonist. Avogadro’s Hypothesis Equal volumes of gases at the same T and P have the same number of molecules. V = n (RT/P) = kn V and n are directly related. twice as many molecules Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gases and Stoichiometry 2 H2O2(liq) ---> 2 H2O(g) + O2(g) Decompose 1.1 g of H2O2 in a flask with a volume of 2.50 L. What is the pressure of O2 at 25 oC? Of H2O? Solution Strategy: • Calculate moles of H2O2 and then moles of O2 and H2O. • Finally, calc. P from n, R, T, and V. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gases and Stoichiometry 2 H2O2(liq) ---> 2 H2O(g) + O2(g) Decompose 1.1 g of H2O2 in a flask with a volume of 2.50 L. What is the pressure of O2 at 25 oC? Of H2O? Solution 0.016 mol of O2 P of O2 = nRT/V (0.016 mol)(0.0821 L• atm/K • mol)(298 K) = 2.50 L P of O2 = 0.16 atm Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gases and Stoichiometry 2 H2O2(liq) ---> 2 H2O(g) + O2(g) Solution What is P of H2O? Calculate as above, or recall Avogadro’s hypothesis. V n at same T and P P n at same T and V 2 times as many moles of H2O as of O2. P n. P of H2O is 2X P of O2. P of H2O = 0.32 atm Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Dalton’s Law of Partial Pressures 2 H2O2(liq) ---> 2 H2O(g) + O2(g) 0.32 atm 0.16 atm What is the total pressure in the flask? Ptotal in gas mixture = PA + PB + ... Therefore, Ptotal = P(H2O) + P(O2) = 0.48 atm Dalton’s Law: total P is sum of PARTIAL pressures. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved