EMR info Waves, light, and energy: Where chemistry and physics collide http://imagers.gsfc.nasa.gov/ems/waves3.html First things first: Waves a and b represent wavelength (λ)- the distance of a wave from crest to successive crest; measured in meters http://www.lbl.gov/MicroWorlds/ALSTool/EMSpec/EMSpec.html Waves: amplitude n The height of a wave from crest to midline or trough to midline; measured in meters Terms you need to know: n Wavelength (λ) Amplitude n Frequency (v; I know some of you have n used f, move on and get with chemisty!): ¡ the number of cycles per second n n measured in cycles per second (s-1) or Hz (Hertz) Propagation of electromagnetic waves http://www.lbl.gov/MicroWorlds/ALSTool/EMSpec/EMSpec2.html http://micro.magnet.fsu.edu/primer/lightandcolor/images/electromagneticfigure1.jpg http://lepus.physics.ualr.edu/~tahall/EXAM2/emspec.jpg http://www.arpansa.gov.au/images/emsline2.gif Visible Light n n n n n n n n colour wavelength(Å) f(*1014 Hz) Energy (*10-19 J) Violet 4000---4600 7.5--6.5 5.0--4.3 Indigo 4600---4750 6.5--6.3 4.3--4.2 Blue 4750---4900 6.3--6.1 4.2--4.1 Green 4900---5650 6.1--5.3 4.1--3.5 Yellow 5650---5750 5.3--5.2 3.5--3.45 Orange 5750---6000 5.2--5.0 3.45--3.3 Red6000---8000 5.0--3.7 3.3--2.5 Some equations you need to know n n n n λ= c / v and E = hv So…. E = hc / λ And… λ = h / mv When • λ= wavelength in m • c = speed of light, 3.00E8 m/s • v = frequencyin Hz • (cycles/sec or s-1 or 1/s) • E= energy in J • h= Plank’s constant, 6.626E-34 J*s [Joule(seconds)] • m= mass of particle in kg What the h? Planck’s Constant n n n When metals are heated, they glow 1800s- physicists were trying to determine the relationship between the color (wavelength) and intensity of the glow Max Planck (1900)- energy can be released or absorbed only in little chunks (packets) of energy “of some minimal size” Max Planck and the h n n The chunks of energy were dubbed “quantum” (“fixed amount”), which is the smallest amount that can be emitted or absorbed as EMR. Proposed: E = hv ¡ The energy (E) of a single quantum is equal to its frequency (v) times a constant Planck and the Nobel (Physics) n n n n n Planck determined that h= 6.626E-34 J-s Energy is always released in multiples of hv (1hv, 2hv, 3hv, etc) H is so small that we cannot see the effects of this in our daily lives Analogous to… Planck won the 1918 Nobel Prize in physics for his work Einstein & Bohr: Perfect Together Einstein (or Mr, Read, you decide), left Bohr, above Einstein: The Photoelectric Effect n n Einstein discovered that one could cause electrons to be ejected from the surface of a metal if the energy of the light wave was strong enough He treated the light needed to do this as a piece of matter- a photon, if you will n This ejection of eis the photoelectric effect The Photoelectric Effect n Only light of a certain energy could knock off an electron from the metal ¡ ¡ n Intense light of a weaker wavelength would not work, but even a low intensity of the correct wavelength would work (the energy of the light is transferred to the kinetic energy of the electron) Hmmm… light acting as a particle and as a wave….. The photoelectric effect… n n http://www.lewport.wnyric.org/ mgagnon/Photoelectric_Effect/ photoelectriceffect1.htm http://www.xmission.com/~locutus/ applets/Photoelectric.html Getting to Bohr…. n n Light of a given wavelength is monochromatic (one color) Most common EMR sources are polychromatic, but we see only one color ¡ These can be reduced to a spectrum when the different wavelengths are separated out Spectral Emissions n Continuous spectrum: shows all colors of the rainbow n n Bright line spectrum: only certain wavelengths are visible (the rest do not appear at all) Different elements have different bright line spectrum when they are heated ¡ ¡ Na is yellow Ne is orange-red Line spectrum n Ne n I2 http://www.cartage.org.lb/en/themes/Sciences/Astronomy/Modenastronomy/Interactionoflight/AtomicAbsorption/AtomicAbsorption.htm Hydrogen Spectra Emission Spectra Absorption Spectra http://www.mhhe.com/physsci/astronomy/applets/Bohr/content_files/section1.html http://www.cartage.org.lb/en/themes/Sciences/Astronomy/Modenastronomy/Interactionoflight/AtomicAbsorption/AtomicAbsorption.htm n Line spectra formation- go to….. http://www.mhhe.com/physsci/ chemistry/essentialchemistry/flash/ linesp16.swf Bohr Model and Spectral Emissions n Bohr proposed that the emission of light energy from an (electrically or thermally) excited atom corresponds to the orbit of the electron around the nucleus of the atom ¡ That energy can only be achieved by being a specific distance from the nucleus What you’ve seen so far…. Model of a Nitrogen (z=7) atom Bohr Model and moving electrons n http:// www.colorado.edu/ physics/2000/ quantumzone/ bohr.html Energy levels- Bohr Model n n Electrons travel within set energy levels that have a particular energy associated with each level After all, the e-s are moving around the nucleus ¡ n think KE here Each shell has a number ¡ ¡ Closest to the nucleus is n=1 For each successive level add 1 to n n n=2, n=3, ect…. Energy increases as the distance from the nucleus increases Bohr Model and moving electrons n http:// www.colorado.edu/ physics/2000/ quantumzone/ bohr.html Electron config in energy level SO… n n We know that the e-s are free to move around the nucleus They also can move from one energy level to the next (and fall) back when energy is added ¡ ¡ Move from ground state (“home” level) to a higher level (the “excited” state) Returning back to the ground state releases energy n This emission is how we see colors: ¡ the wavelengths of EMR released from an atom when it has been excited by n n n ¡ Heat energy Electrical energy Chemical energy Think glowing red hot metal, or fireworks Also…life after Einstein and Bohr n We know that electrons have characteristics of both light (waves) and matter so we say that they have a dual nature De Broglie n De Broglie proposed that an electron moving about the nucleus had a wave-like behavior, so that they it has a particular wavelength associated with it. This wavelength depends upon the mass and velocity of the electron. ¡ λ = h / mv ¡ mv = the momentum of the particle n n n This matter-wave idea applies to all matter, not just to electrons However, the mass is so large, and the wavelength so small, that we cannot see it in macroscale objects This matter-wave theory led to applications like the electron microscope De Broglie wavelength EMR and the atom: Part Deux Electron Configurations: from waves to orbitals http://imagers.gsfc.nasa.gov/ems/waves3.html Heisenberg: The Uncertainty Principle n We can’t determine information about small scale objects the same way we can for large scale objects ¡ ¡ Case in point: a ball rolling down a rampwe can get position, direction, and speed at the same time We can’t for electrons n Hence, the uncertainty principle Heisenberg, cont’d n n n n It is inherently impossible for us to simultaneously know both the exact momentum and exact location of an electron This is because anything we do to determine the location or momentum of the electron moves it from its original path and location; this can’t be reduced past a certain minimal level We can know only momentum or location- not both We can talk probability of the location/ momentum of an electron Which brings us to this question: n What the heck does all of this have to do with electron configuration and how matter behaves? ¡ On to electron configuration, courtesy of SchrÖdinger and company (enter math that we’ll skip because we don’t have enough time or energy to devote to this) n Quantum theory: Treats e-s as quantized particle-waves of energy that orbit the nucleus in set paths ¡ Therefore, each location for an e- has a set energy EMR and the atom: Part Deux Electron Configurations: from waves to orbitals http://imagers.gsfc.nasa.gov/ems/waves3.html Warning: n n Much of what we do will not make sense until it is all put together Use what we are going now as rules for what we are going to do with this information, and know that the problems are not in this packet The Bohr Model: What you’ve seen so far in life General tutorials for electron configuration stuff n n n some slides in this PowerPoint are from this site already http://www.wwnorton.com/chemistry/ overview/ch3.htm See key equations and concepts (select from menu on the left), as well as the looking through the overview where to the tutorials are listed (links for just those are on the left, too) What you’ve seen so far…. Model of a Nitrogen (z=7) atom Which is really not true- why? n Because orbitals- the “electron cloud” are 3-D, not flat ¡ are not round in most cases ¡ e-s are spread out as much as possible ¡ (e-s are moving very rapidly) ¡ Orbitals n The electrons are spread out in orbitals that have varying ¡ ¡ n Shapes Energy (distance from nucleus) The orbitals are described in regards to their quantum numbers ¡ ¡ Descriptions that are descriptive and hierarchical There are 4 numbers that describe an orbital n Written as follows: (#, #, #, ±#) Principal quantum number (n) The first number (1, #, #,±#) n Describe the ¡ ¡ n Values for n are integers ¡ n distance from the nucleus of the orbital The energy of the orbital The smallest possible value is 1 As the distance from the nucleus (and therefore energy) increases, the number increases Quantum numbers The periodic table and n n n The 7 periods on the periodic table correspond to n values Each period has a unique n value ¡ ¡ ¡ For the 1st period, n=1 For the 2nd period, n=2 And so on…. Angular Momentum (l) (this is a script l, as in llama) n n n Is the shape of the orbital It is the second number in the description (#, 1,#, ±#) Range from 0 to n-1 (although we never deal with anything above l=3) ¡ ¡ ¡ ¡ s =0 p =1 d =2 f=3 The s orbital l=0 http://www.sfu.ca/~nbranda/28xweb/images/s_orbital.gif p orbitals l=1 d orbitals l=2 Another look at d orbitals f orbitals l=3 Blocks and l The blocks you already know correspond to the orbital of the last (outermost) e- , or valence e-s occupies Magnetic number (ml) n n Denote the orbital sublevel that is filled It is the third number in the description (#,#, 1, ±#) ¡ ¡ ¡ ¡ s orbitals have one sublevel; a sphere has one orientation in space p orbitals have three sublevels; 3 orientations in space d orbitals have five sublevels; 5 orientations in space f orbitals have seven sublevels; 7 orientations in space “Flavors” of ml n s orbitals have one sublevel; a sphere has one orientation in space “Flavors” of ml n p orbitals have three sublevels; 3 orientations in space “Flavors” of ml n d orbitals have five sublevels; 5 orientations in space “Flavors” of ml n f orbitals have seven sublevels; 7 orientations in space Magnetic number (ml) n n n n Denote the orbital sublevel that is filled It is the third number in the description (#,#, 1, ±#) Values of –l to l, (integers only) For ¡ ¡ ¡ ¡ s p d f ml = 0 only since l= 0 ml = -1,0,1 since l= 1 ml = -2,-1,0,1,2 since l= 2 ml = -3,-2,-1,0,1,2,3 since l= 3 Spin n n It is the last number in the description (#,#,#,±½) Spin is +½ or -½ ¡ Up or down Summary, excluding spin How we use this…. n There is a specific order to how the efill the orbitals; it is not random ¡ Although there are exceptions to the rules (which is the last thing we’ll do; pretend for this moment that everything follows these rules, as most elements do) The principles of econfiguration n The Aufbau (next) Principle: ¡ n The Pauli Exclusion Principle: ¡ n That e- fill the lowest energy sublevel before going to the next sublevel That e-s are paired according to opposite spins Hund’s Rule: ¡ e-s spread out in equal energy sublevels before placing electrons in the next level n The first level to fill is the 1s level ¡ ¡ It is the lowest energy sublevel It holds two electrons n n They are oppositely paired (up and down- ↑↓) Each sublevel (each __) holds 2 electrons Next… n n The second sublevel is the 2s sublevel It also holds 2 electrons ¡ n because s orbitals have one sublevel, (not 2 electrons because of the number 2)* also oppositely paired ↑↓ *the number is n=, so the number tells how far form the nucleus, not the number of sublevels or electrons it holds 1s2, 2s2,then comes 2p6 n So, as it states above ¡ 1s fills, 2s fills ,then comes 2p n n It holds up to six electrons Because p orbitals hold 6 electrons in 3 sublevels (_ _ _) Next… n From 2p, ¡ ¡ ¡ ¡ ¡ n n 3s fills with 2e-, then onto 3p, with 6e- then 4s with 2e- followed by 3d with 10e- (because d holds 10e-) Then 4p with 6e- Notice, you follow the arrows Remember, the number of electrons comes from the letter (the orbital’s momentum, m) n n n The sublevels of the orbitals are first filled, then you continue onto the next level (Aufbau) Also be sure to place one electron in each sublevel prior to filling the level (↑ ↑ ↑ and not ↑↓ ↑ _) (Hund) e-s must be paired with e-s of opposite spin (↑↓, not ↑↑ or ↓↓) (Pauli) Putting it all together… n n Carbon (neutral, so 6 electrons) What this would look like: ↑↓ ↑↓ ↑ ↑ _ 1s 2s 2p (notice there are 6 arrows for 6 electrons) n n This can also be written as 1s2 2s2 2p2 Notice the superscripts add up to 6 There are some exceptions… n This is because some energy levels are very close together ¡ n n electrons are able to move between close orbitals in order to minimize repulsion Example: the 4s and 3d orbitals are very close in energy So exceptions for some period 4 d block elements occur ¡ ¡ ¡ Cr is not 1s2 2s2 2p6 3s2 3p6 4s2 3d4 Cr is 1s2 2s2 2p6 3s2 3p6 4s1 3d5 Because it takes less energy to split the electrons between the 5 sublevels than it does to put them together in the 4s and 3d Electron configurations Abbreviated e- configurations Orbital diagrams