atomic spectroscopy
DESCRIPTION
Reviewer for Atomic SpectroscopyTRANSCRIPT
Atomic Spectroscopy
An Introduction of Spectrometric Methods
Properties of Electromagnetic Radiation
Electromagnetic Radiation– energy radiated in the form of a WAVE caused
by an electric field interacting with a magnetic field
– result of the acceleration of a charged particle– does not require a material medium and can
travel through a vacuum
Properties of Electromagnetic Radiation
vi = i
where vi => velocity => frequency i => wavelength
Properties of Electromagnetic Radiation
in vacuum, velocity is independent of frequency,
maximum value
c =
= 2.998 X 108 m/s
Properties of Electromagnetic Radiation
"Representation of a beam of monochromatic, plane polarized radiation. The arrows represent the electrical vectors."
Properties of Electromagnetic Radiation
"Effect of change of medium on a monochromatic beam of radiation."
Properties of Electromagnetic Radiation
"Regions of the electromagnetic spectrum"
Properties of Electromagnetic Radiation
"Common Spectroscopic Methods Based on electromagnetic Radiation"
Properties of Electromagnetic Radiation
Wave Equationfor a single wave
y = A sin (2t + )
Properties of Electromagnetic Radiation
for n waves of same frequency superimposed of phase angle y = A1 sin (2t + 1 )
+ A2 sin (2t + 2 )+ A3 sin (2t + 3 )+ + An sin (2t + n )
Properties of Electromagnetic Radiation
"Superposition of sinusoidal waves: (a) same frequency, small difference in phase (b) same frequency, large difference in phase (c) difference frequencies, starting in phase.
Properties of Electromagnetic Radiation
for n waves of different frequencies superimposed of phase angle y = A1 sin (2
t + 1 )+ A2 sin (2
t + 2 )+ A3 sin (2
t + 3 )+ + An sin (n t + n )
Properties of Electromagnetic Radiation
"Superposition of sine waves to form a square wave: (a) combination of three sine waves, and (b) combination of three, as in (a), and nine sine waves."
Diffraction
"Propagation of waves through a slit: (a) xy >(b) xy ."
Diffraction
"Diffraction of monochromatic radiation by slits."
Diffraction
= CF = BC sin
n
= CF = BC sin
DE = OD sin
DiffractionBC DE BC DE
n = ---------- = ------------OD OE
where OE => distance from screen to plane of slitsBC => slit spacingDE => band spacing
EXAMPLE: Suppose that the screen in the figure shown is 2.00 m from the plane of the slits and that the slit spacing is 0.300 mm. What is the wavelength of radiation if the fourth band is located 15.4 mm from the central band?
EXAMPLE: Suppose that the screen in the figure shown is 2.00 m from the plane of the slits and that the slit spacing is 0.300 mm. What is the wavelength of radiation if the fourth band is located 15.4 mm from the central band?
BC DE BC DEn
= ------------ = ------------
OD OEn = 4
___OE = 2.00 m___BC = 0.300 mm___DE = 15.4 mm
EXAMPLE: Suppose that the screen in the figure is 2.00 m from the plane of the slits and that the slit spacing is 0.300 mm. What is the wavelength of radiation if the fourth band is located 15.4 mm from the central band?
n = 4 OE = 2.00 m___ ___BC = 0.300 mm DE = 15.4 mm
(0.300 mm)(15.4 mm) = ----------------------------
4 (2 * 1000)mm= 5.78 X 10-4 mm or 578 nm
Transmission of RadiationTransmission
– rate at which radiation passes through a transparent material is less than through a vacuum
– depends upon the kinds and concentrations of atoms, ions, and molecules in the medium
– radiation must interact with material– interaction must not undergo permanent energy
transfer
Transmission of Radiation
Transmissionni = c/vi
where ni => refractive index, measure of interactionc => speed of light in vacuumvi => speed of light in medium
Transmission of Radiation
Dispersion– variation in refractive index of a substance with
wavelength or frequencyRefraction of Radiation
– Snell’s Law
sin
n2 v1
sin
n1 v2
Reflection of Radiation
• reflection always occurs when radiation passes from one medium to another
• reflection greatest when two materials have the greatest difference on their refractive indices
Scattering of Radiation
Types of Scattering– Rayleigh Scattering
• scattering involving molecules which are considerably smaller than the wavelength of radiation
• blue sky results from greater scattering of shorter wavelength visible light
Scattering of Radiation
Types of Scattering– Scattering by Large Molecules
• can be measured• a function of the size and shape of molecule
Scattering of Radiation
Types of Scattering– Raman Scattering
• part of the radiation undergoes quantized frequency changes
Quantum-Mechanical Properties of Radiation
E = h
= hc/
Emission of Radiation
• Line spectra• Band spectra• Continuum spectra
Line spectra
“Emission spectrum of a brine obtained with an oxy-hydrogen flame”
Line spectra
“X-ray emission spectrum of Molybdenum metal”
Band spectra
“Energy-level diagram for (a) a sodium atom showing the source of a line spectrum and (b) a simple molecule showing the source of a band spectrum.”
Continuum spectra“Blackbody radiation curves”
Absorption of Radiation
energy of exciting photon must equal energy difference between ground state and 1 excited state for absorption to occur
Absorption of Radiation
"Some typical ultraviolet absorption spectra."
Atomic Absorption
• absorption occurs with only a few well- defined frequencies
• electronic excitation
Molecular Absorption
E = Eelectronic + Evibrational + Erotational
Molecular Absorption
"Partial energy level diagram for a fluorescent organic molecule."
Emission of Radiation
• radiation resulting from the relaxation to lower energy states of excited particles
Absorption Methods, Transmittance
T = P/Po
where T => transmittanceP => power of transmitted radiationPo => power of incident
radiation%T = (P/Po )*100
where %T => percent transmittance
Absorption Methods, Absorbance
A = - log10 T = - log10 (P/Po )
where A => absorbance
Absorption Methods, Beer’s Law
A = abc = bcwhere a => absorptivity
b => path lengthc => concentration
=> molar absorptivity
Spectroscopic Methods
“Major classes of spectroscopic methods”
Absorption Methods
“Attenuation of a beam of radiation by an absorbing species”
Absorption Methods“Single-beam photometer for absorption measurements in the visible region.”
Absorption Methods“Readout for an inexpensive photometer.”
transmittance scale is linearabsorbance scale is exponentialthus, read transmittance, then calculate absorbance