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1 Chem 1211 Class 14 Atomic Structure Chapter 6 © 2009 Brooks/Cole - Cengage Arrangement of Electrons in Atoms Electrons in atoms are arranged as SHELLS (n) SUBSHELLS (l) ORBITALS (ml) © 2009 Brooks/Cole - Cengage 2 QUANTUM NUMBERS There is a hierarchy in quantum numbers: A few different l can exist for the same n and a few different ml can exist for the same l • n determines the energy of the orbital • for hydrogen atom the energy of the orbital does not depend on l and ml • l determines shape of the orbital • ml determines position of the orbital relative to others with the same l © 2009 Brooks/Cole - Cengage 3 Azimuthal Quantum Number • l determines the shape of the orbital • for given n, l can be any integer from 0 to (n-1) • every l has its proper (letter) name: orbital with l = 0 called s-orbital orbital with l = 1 called p-orbital orbital with l = 2 called d-orbital orbital with l = 3 called f-orbital © 2009 Brooks/Cole - Cengage 4 Magnetic Quantum Number • ml determines position of the orbital relative to others with the same l and how many orbitals with the same l can exist. • ml is an integer from - l to l, so for given l, there are (2l +1) orbitals with different ml l =0 l =1 l =2 l =3 © 2009 Brooks/Cole - Cengage s-orbital p-orbital d-orbital f-orbital How many? 1 3 5 7 5 6 Types of Atomic Orbitals 2px n, principal l, azimuthal ml, magnetic See Active Figure 6.14 © 2009 Brooks/Cole - Cengage Arrangement of Electrons in Atoms: restriction on number of residents! 7 Each orbital can be occupied by no more than 2 electrons! Because: No two electrons in atom can have the same set of all quantum numbers (Pauli’s Exclusion Principle) And: Wolfgang Pauli (1900-1958) There is a 4th quantum number, the electron spin quantum number, ms. © 2009 Brooks/Cole - Cengage Electron Spin Quantum Number, ms 8 • Can be proven experimentally (Stern, Gerlach, 1926) that electron has a magnetic moment (acts as a small magnet). • It referred to as “spin.” • Spin is quantized: it can be only along magnetic field or against magnetic field. • Two spin directions are given by ms = +1/2 and -1/2. © 2009 Brooks/Cole - Cengage Electron Spin Quantum Number, ms 9 • If two electrons in atom have the opposite spins, the total spin is zero (spins are “paired”) • Electron spin is responsible for magnetic properties of the materials • Materials containing unpaired spins are either paramagnetic or ferromagnetic • Materials containing only paired spins are diamagnetic © 2009 Brooks/Cole - Cengage Electron Spin and Magnetism •Diamagnetic: NOT attracted to a magnetic field (slightly repelled) •Paramagnetic: substance is attracted to a magnetic field. •Ferromagnetic: substance is strongly attracted to a magnetic field. •Substances with unpaired electrons are paramagnetic or ferromagnetic. © 2009 Brooks/Cole - Cengage 10 Measuring Paramagnetism Paramagnetic: substance is attracted to a magnetic field. Substance has unpaired electrons. Diamagnetic: NOT attracted to a magnetic field See Active Figure 6.18 © 2009 Brooks/Cole - Cengage 11 12 magnetic field ferromagnetic © 2009 Brooks/Cole - Cengage diamagnetic paramagnetic 13 QUANTUM NUMBERS Now there are four! n → shell 1, 2, 3, 4, ... l → subshell 0, 1, 2, ... n - 1 ml → orbital - l ... 0 ... + l ms → electron spin +1/2 and -1/2 © 2009 Brooks/Cole - Cengage Magnetic Resonance Imaging (MRI) Protons and neutrons are also small magnets, means, they also have spin; Proton is the nucleus of hydrogen, energy transitions of its spin in strong magnetic field can be measured by Nuclear Magnetic Resonance (NMR); Concentration of the protons (i.e. water) in different parts of the sample can be measured by NMR - that is called Magnetic Resonance Imaging (MRI) It is powerful diagnostic tool, because living organism mostly consists of water! © 2009 Brooks/Cole - Cengage 14 15 Magnetic Resonance Imaging (MRI) X-Ray © 2009 Brooks/Cole - Cengage MRI 16 Chem 1211 Atomic Electron Configurations and Periodic Table Chapter 7 © 2009 Brooks/Cole - Cengage Arrangement of Electrons in Atoms Electrons in atoms are arranged as SHELLS (n) SUBSHELLS (l) ORBITALS (ml) © 2009 Brooks/Cole - Cengage 17 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 and… © 2009 Brooks/Cole - Cengage 18 19 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. © 2009 Brooks/Cole - Cengage When n = 1, then l = 0 this shell has a single orbital (1s) to which two e- can be assigned. first shell Electrons in Atoms 20 2s orbital 2e- three 2p orbitals 6e- TOTAL = 8e- © 2009 Brooks/Cole - Cengage second shell When n = 2, then l = 0, 1 Electrons in Atoms © 2009 Brooks/Cole - Cengage 2e6e10e18e- third shell When n = 3, then l = 0, 1, 2 3s orbital three 3p orbitals five 3d orbitals TOTAL = 21 Electrons in Atoms When n = 4, then l = 0, 1, 2, 3 4s orbital three 4p orbitals five 4d orbitals seven 4f orbitals TOTAL = And many more! 2e6e10e14e32e- In general, electron capacity of n-th shell is 2n2 © 2009 Brooks/Cole - Cengage 22 ATOMIC ELECTRON CONFIGURATIONS23 AND PERIODICITY Length of period corresponds to shell capacity only for the 1st two periods. WHY? © 2009 Brooks/Cole - Cengage Assigning Electrons to Atoms • Electrons generally assigned to orbitals of successively higher energy. • For H atoms, E = - C(1/n2). E depends only on n. • For many-electron atoms, energy depends on both n and l. • See Active Figure 7.1 and Figure 7.2 © 2009 Brooks/Cole - Cengage 24 Assigning Electrons to Subshells • In H atom all subshells of same n have same energy. • In many-electron atom: a) subshells increase in energy as value of n + l increases. b) for subshells of same n + l, subshell with lower n is lower in energy. © 2009 Brooks/Cole - Cengage 25 Aufbau scheme: electrons occupy the position with the 26 lowest possible energy Electron Filling Order See Figure 7.2 Why is this order? © 2009 Brooks/Cole - Cengage Effective Nuclear Charge, Z* • Z* is the nuclear charge experienced by the outermost electrons. See Figure 7.3 • Explains why E(2s) < E(2p) • Z* increases across a period owing to incomplete shielding by inner electrons. • Estimate Z* = [ Z - (no. inner electrons) ] • Charge felt by 2s e- in Li Z* = 3 - 2 = 1 • Be Z* = 4 - 2 = 2 • B Z* = 5 - 2 = 3 and so on! © 2009 Brooks/Cole - Cengage 27 28 Effective Nuclear Charge See Figure 7.3 Z* is the nuclear charge experienced by the outermost electrons. Electron cloud for 1s electrons © 2009 Brooks/Cole - Cengage 29 Effective Nuclear Charge probability distribution for 2p electron Shielding by inner electrons: s < p < d Effective charge for s > p > d Correspondingly, energy: s < p < d © 2009 Brooks/Cole - Cengage See Figure 7.3 Z* is the nuclear charge experienced by the outermost electrons. Aufbau scheme: electrons occupy the position with the 30 lowest possible energy Electron Filling Order See Figure 7.2 Now we understand the order! © 2009 Brooks/Cole - Cengage Writing Atomic Electron Configurations Two ways of writing configs. One is called the spdf spdf notation for H, atomic number = 1 notation. 1 1s value of n © 2009 Brooks/Cole - Cengage no. of electrons value of l 31 Writing Atomic Electron Configurations Two ways of writing configs. Other is called the orbital box notation. ORBITAL BOX NOTATION for He, atomic number = 2 Arrows 2 depict electron spin 1s 1s One electron has n = 1, l = 0, ml = 0, ms = + 1/2 Other electron has n = 1, l = 0, ml = 0, ms = - 1/2 © 2009 Brooks/Cole - Cengage 32 33 See “Toolbox” in ChemNow for Electron Configuration tool. © 2009 Brooks/Cole - Cengage characteristic elements Electron Configurations and the Periodic Table © 2009 Brooks/Cole - Cengage 34 See Active Figure 7.4 Lithium Group 1A Atomic number = 3 1s22s1 → 3 total electrons 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage 35 36 Beryllium 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage Group 2A Atomic number = 4 1s22s2 → 4 total electrons Boron 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage Group 3A Atomic number = 5 1s2 2s2 2p1 → 5 total electrons 37 Carbon 38 Group 4A Atomic number = 6 1s2 2s2 2p2 → 6 total electrons 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage Here we see for the first time HUND’S RULE. When placing electrons in a set of orbitals having the same energy, we place them singly as long as possible (maximal spin configuration has the lowest energy). 39 Nitrogen 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage Group 5A Atomic number = 7 1s2 2s2 2p3 → 7 total electrons 40 Oxygen 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage Group 6A Atomic number = 8 1s2 2s2 2p4 → 8 total electrons 41 Fluorine 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage Group 7A Atomic number = 9 1s2 2s2 2p5 → 9 total electrons 42 Neon Group 8A Atomic number = 10 1s2 2s2 2p6 → 10 total electrons 3p 3s 2p 2s 1s © 2009 Brooks/Cole - Cengage Note that we have reached the end of the 2nd period, and the 2nd shell is full!