Title | Wlesson 3 Sp 2020 electromagnetic spectra and atomic spectra |
---|---|
Course | General Chemistry I |
Institution | University of Illinois at Urbana-Champaign |
Pages | 29 |
File Size | 1.1 MB |
File Type | |
Total Downloads | 8 |
Total Views | 171 |
stuff for general chemistry for kelly marville...
ELECTROMAGNETICRADIATION ANDBOHRMODELOFTHEATOM Pleasespendextratimeunderstandingandlearningthematerialontheslideswith*
DimensionalAnalysis Theprocessofunitconversionisfacilitatedusingdimensionalanalysis. Unit factors are utilized in this process and are made from any two equivalent factors. StudentProblem(thisproblemwillnotbedoneinlecture) Convert619nmtomknowingthat109nm=1m
ElectromagneticRadiationandElectromagneticSpectrum • Electromagnetic radiation is the emission and absorption of energy in the form of electromagnetic waves. This type of energy therefore has wavelength, frequency and speed.
• Theelectromagneticspectrumisacontinuous (uninterrupted)band ofvisibleandinvisiblelightthatrangesfromshorttolong wavelengths.
ElectromagneticSpectrum
Wavelength,FrequencyandAmplitude
* Wavelength (symbol: , pronounced lambda, units: m) is the distance between two peaks or troughs in the wave. Frequency (symbol: , pronounced nu, units: s‐1 which is called Hz) is the number of wavelengths per second that travel past a given point. Amplitude: Vertical distance from the midline of a wave to the peak or trough.
RelationshipbetweenFrequencyandWavelength
*
The product of frequency () and wavelength () always equals a constant, c, the speed of light:
c= c=2.998x108m/s
Attimes,cisrequiredintermsofnm:c=2.998x1017 nm/s
As frequency increases, the wavelength decreases; thus they are inversely related.
Problem A radio station broadcasts at 580. kHz. What is the wavelength (in meters) of this radio signal ? c = 2.998 x 108 m/s
1000 Hz = 1kHz
,units:s‐1 whichiscalledHz
c=
QuantizedEnergyAnalogy Quantum: The smallest quantity of energy that can be emitted or absorbed in the form of electromagnetic radiation. ContinuousEnergy:Anyamountofenergycanbemeasured. Energyisquantized:onlycertainenergiesareallowed. A ramp is analogous to continuous energy – you can sit at any position along a ramp and thus be at any elevation between the two levels. Stairs, however, are analogous to quantized energy – you can only sit at certain elevations between the two levels and nowhere in between. You may sit only on the steps, not in between the steps. Only certain elevations are allowed.
QuantizedEnergy
*
Max Planck postulated that energy could be gained or lost only in whole number multiples of the quantity h .
He related the energy of radiation emitted or absorbed to its frequency using the equation:
Planck’sEquation: Energyof radiation(J)
E=h
frequency
Planck’sconstant (h=6.626x10‐34J•s) (h=6.626x10‐34kg•m2/s)
Note:SometexthaveE=nh wherenisapositiveinteger(1,2,3,etc.)calledaquantumnumber
QuantizedEnergy
*
• Each change in an atom’s energy occurs when the atom absorbs or emits one or more “packets” of energy. Each packet is called a quantum.
•
A quantum of energy is equal to h .
• An atom changes its energy state by emitting (or absorbing) one or more quanta (plural of quantum), and the energy of the emitted (or absorbed) radiation is equal to the difference in the atom’s energy states, i.e. E = h .
EnergyasParticles
*
Albert Einstein proposed that electromagnetic radiation is itself quantized and can be viewed as a stream of “particles” called photons.
• Hededucedtheenergyofaphotonusing:
• Note that energy is inversely related to wavelength, and directly related to frequency.
Problem An electron emitted light having an energy of 3.025 x 10‐19 J. What is the wavelength of this light in nm? h=6.626x10‐ 34J•s,c=2.998x1017 nm/s,E=h =h(c/)
DualNatureofLight
*
• Einstein and Planck proved that electromagnetic radiation exhibits wavelike AND particulate properties (wave‐particle duality). • de Broglie then proved that matter exhibits particulate AND wavelike properties. • Foraparticlewithvelocity,u:
• Wavelengthofaparticle: deBroglie’sEquation
Problem What is the deBroglie’s wavelength (in m) of a 142 g baseball thrown at 44 m/s?
h=6.626x10‐ 34J•s,1J=1kg(m2/s2), =h/(mu) ,1000g=1kg
Whatdowenowknowaboutmatterandenergy? MatterandenergyareNOTdistinct. Energy is a form of matter and all matter exhibits both the properties of waves AND of particles. Large pieces of matter exhibits particulate properties with an associated wavelength that is so small that it is not observed. Its wave‐like properties are not considered. Small pieces of matter exhibit wave properties predominantly and some particulate properties.
Bohr’sModeloftheAtom ContinuousSpectrum
white light prism
White light passed through a prism produces a spectrum of color that contains all of the wavelengths of visible light. This is why the spectrum is called continuous.
LineEmissionSpectrumofHydrogen
*
*
TheBohrModeloftheAtom
Bohrpostulated:
• Theelectroninahydrogenatomcirclesthe
Bohrmodelof hydrogenatom
nucleusoftheatomincircularorbits(energylevels)thatarequantized. • Theenergyoftheelectroninhydrogenisquantizedanddependson theorbititoccupies.
• The energy of the electron in a given orbit is proportional to its distance from the nucleus.
*
TheBohrModeloftheHydrogenAtom:EnergyLevels
• Energylevels:n=1< n=2< n=3... n=1
ground energystate
stable
n>1
excited energystates
unstable
n=∞
electronleavesatom
n= Quantumnumber
LineEmissionSpectrumofHydrogen
*
TransitionsresponsibleforBalmer/visibleseries The Balmer series of lines is caused by electrons dropping from outer orbits to the n = 2 orbit.
Fourlinesinthevisibleregion: • red (656nm)(32) • blue‐green (486nm)(42) • blue‐violet (434nm)(52) • violet(410nm)(62)
These lines provide evidence that changes in energy between discrete energy levels in hydrogen will produce only certain wavelengths of light, i.e. the energy of the electron is quantized.
SpectralLinesEmittedbytheHatom
*
NameofSeries
Causedbyelectrons droppingfromouter orbitsto
LymanorUVseries
n=1orbit
Balmerorvisibleseries
n=2orbit
Paschen orinfrared series
n=3orbit
Brackettseries
n=4orbit
Pfund series
n=5orbit
WhatHappensWhenanElectronAbsorbsEnergy?
* photon Electronabsorbsphoton andgoestoahigherenergy level,inthiscase,n=3
n=1
nucleus n=2 n=3
WhatHappensWhenanElectronEmitsEnergy?
*
Electronemitsphoton andgoestoalower energylevel,inthis case,n=1
photon
n=1
nucleus n=2
n=3
EnergyAbsorptionandEmission Orbitwithenergy,E2
Energyabsorbed= Energyemitted =E2‐ E1
Orbitwithenergy,E1
Whenenergyis
When energy is
absorbed, Ehas
emitted, E has
apositive value.
a negative value.
Frequencyoflightabsorbed= = Frequencyoflightemitted= =
ଶିଵ ୦
ଶିଵ ୦
E=E2 – E1 E=h
CalculatingEnergyChanges
*
The energy change when the electron in a hydrogen atom moves from one energy level to another can be calculated with:
2.178x10‐18J (Ryberg constant)
ni =initialenergylevel nf =finalenergylevel
nuclearcharge=atomicnumber (H=+1)
Problem: What is the wavelength, in nm, of light emitted when the electron in the hydrogen atom moves from n = 4 to n = 2 ? Give your answer to 3 sig. figs.
ΔE=‐ 2.178x10 – 18JZ2
1 1 nf2 ni2
E=h =hc/ h=6.626x10‐ 34J•s c=2.998x1017 nm/s
CalculatingEnergyChanges
* Thisequationcanonlybeusedforoneelectronspecies,likehydrogen.
Example:He+ andC5+ bothhaveoneelectron,thereforethisformulacould beusedtocalculateenergychanges.ThevalueofZthatwouldbeusedin thisformulaforHe+ andC5+ wouldbe+2and+6,respectively.
LineSpectra
He Ne Na Hg Everyelementhasauniquelineoremissionspectrum
Bohr’sModeloftheAtomisFundamentallyIncorrect
*
Bohr’s model cannot account for the emission spectra of atoms containing more than one electron. Thismodelonlyworksfor1electronsystems. Example:H,He+,Li2+,etc.
It is important to note however, that the current theory of atomic structure, despite not being derived from the Bohr model, does include his postulate that the energy levels in atoms are quantized....