Spectroscopy radiation by atoms Absorption: Low energy electrons absorb energy to move to higher energy level Emission: Excited electrons return to lower energy states Absorption vs.. Em
Trang 1PHAM VAN HUNG, PhD
INTRODUCTION
• The study how the chemical compound interacts with different wavelenghts in a given region of
electromagnetic radiationis called spectroscopy
or spectrochemical analysis
• The collection of measurements signals (absorbance) of the compound as a function of electromagnetic radiation is called a spectrum
Spectroscopy
radiation by atoms
Absorption:
Low energy electrons absorb energy to move to higher energy level
Emission:
Excited electrons return to lower energy states
Absorption vs Emission
Ground State
1st 2nd 3rd
Energy is absorbed as electrons jump to higher energy levels
Energy is emitted by electrons returning to lower energy levels Excited
States
Spectroscopic Techniques
• UV-Visible Spectroscopy (UV-Vis).
• Infrared Spectroscopy (IR)
• Atomic Absorption Spectroscopy (AAS).
• Colorimetry.
UV radiation and Electronic Excitations
• The difference in energy between molecular bonding, non-bonding and anti-non-bonding orbitals ranges from 125-650 kJ/mole
• This energy corresponds to electromagnetic radiation in the ultraviolet (UV) region, 100-350 nm, and visible (VIS) regions 350-700 nm of the spectrum
• For comparison, recall the electromagnetic spectrum:
• Using IR we observed vibrational transitions with energies
of 8-40 kJ/mol at wavelengths of 2500-15,000 nm
UV
γ-rays Microwave Radio
Visible
Trang 2X-ray:
core electron
excitation
UV:
valance
electronic
excitation
IR:
molecular vibrations
Radio waves:
Nuclear spin states (in a magnetic field) Electronic Excitation by UV/Vis Spectroscopy :
3-D structure Anaylysis X-rays
X-ray Crystallography
Elemental Analysis X-rays
X-Ray Spectroscopy
Structure determination Radio waves
FT-NMR
Functional Group Analysis/quant IR/UV
Raman
Functional Group Analysis IR/Microwave
FT-IR
Quantitative analysis Beer’s Law UV-vis region
Atomic Absorption
Quantitative analysis/Beer’s Law UV-vis region
UV-vis Spectroscopic Techniques and Common Uses
Different Spectroscopies
• UV/Vis – electronic states of valence e/d-orbital
transitions for solvated transition metals
• Fluorescence – emission of UV/vis by certain
molecules
• FT-IR – vibrational transitions of molecules
• FT-NMR – nuclear spin transitions
• X-Ray Spectroscopy – electronic transitions of
core electrons
Dispersion of Polymagnetic Light with a Prism
P o ly c h ro m a tic
R a y
I n fra re d
R e d
O ra n g e
G re e n
B lu e
V io le t
U ltr a v io le t
m o n o c h ro m a tic
R a y
S L IT
P R IS M
P o ly c h ro m a tic R a y M o n o c h ro m a tic R a y
• Prism - Spray out the spectrum and choose the certain wavelength (λ) that you want by slit.
• In UV spectroscopy, the sample is irradiated with the broad spectrum of the
UV radiation
• If a particular electronic transition matches the energy of a certain band of
UV, it will be absorbed
Electronic Excitation
The absorption of light energy by organic compounds in the
visible and ultraviolet region involves the promotion of
electrons in σ, π, and n-orbitals from the ground state to higher
energy states This is also called energy transition These higher
energy states are molecular orbitals called antibonding
σ *
π*
n
π
σ
Antibonding
Antibonding
Nonbonding Bonding
Bonding
Electronic Molecular Energy Levels
σ * π*
n π σ
Antibonding Antibonding
Nonbonding Bonding Bonding
• For any bond (pair of electrons) in a molecule, the molecular orbitals are a mixture of the two contributing atomic orbitals; for every bonding orbital “created” from this mixing (s, p), there is a corresponding anti-bonding orbital of symmetrically higher energy (s*, p*).
• The lowest energy bonding orbitals are typically the s; likewise, the corresponding anti-bonding s* orbital is of the highest energy.
• p-orbitals are of somewhat higher energy, and their complementary anti-bonding orbital somewhat lower in energy than s*.
• Unshared pairs lie at the energy of the original atomic orbital, most often this energy is higher than p or s (since no bond is formed, there is no benefit in energy).
• The higher energy transitions (σ →σ*) occur a shorter wavelength and the low energy transitions (π→π*, n →π*) occur at longer wavelength.
Trang 3Observed electronic transitions
From the molecular orbital diagram, there are several possible electronic
transitions that can occur, each of a different relative energy:
Energy
σ∗
π σ
π∗
n
σ σ π n n
σ ∗
π ∗
π ∗
σ ∗
π ∗
alkanes carbonyls unsaturated cmpds.
O, N, S, halogens carbonyls
Observed electronic transitions
- Routine organic UV spectra are typically collected from 200-700 nm
- This limits the transitions that can be observed:
σ σ π n n
σ ∗
π ∗
π ∗
σ ∗
π ∗
alkanes carbonyls unsaturated cmpds.
O, N, S, halogens carbonyls
150 nm
170 nm
180 nm √ - if conjugated!
190 nm
300 nm √
UV
Observed electronic transitions
- Remember the electrons present in organic molecules are involved
in covalent bonds or lone pairs of electrons on atoms such as O or N
- A functional group capable of having characteristic electronic
transitions is called a chromophore (color loving).
- Chromophore is a functional group which absorbs a characteristic
ultraviolet or visible region.
C C
C C
C O
C O H
λ A
180 nm
279 nm
C O
Spectrum
Spectrum
Glass cell filled with concentration of solution (C)
I I
Light
0
Transmittance is defined as the ratio of the electromagnetic radiation’s power
exiting the sample, I, to that incident on the sample from the source, I 0,
I
I0
T =
An alternative method for expressing the attenuation of electromagnetic
radiation is absorbance, A, which is defined as
A = - Log T = - Log = Log I0
I I
I0
Transmittance and Absorbance
Trang 4Beer – Lambert Law
• There is a logarithmic dependence between the transmission, T, of light
through a substance and the product of the absorption coefficient of the
substance, α, and the distance the light travels through the material, ℓ
• The absorption coefficient can, in turn, be written as a product of either a
molar absorptivity (extinction coefficient) of the absorber, ε, and the molar
concentrationc of absorbing species in the material.
• The molar absorptivity give, in effect, the probability that the analyte will absorb
a photon of given energy As a result, value for ε depend on the wavelength of
electromagnetic radiation Compound x has a unique e at different wavelengths.
• Unit of ε: L*cm -1 *M -1
Steps in Developing a Spectrometric Analytical Method
1 Run the sample for spectrum
2 Obtain a monochromatic wavelength for the maximum absorption wavelength
3 Calculate the concentration of your sample using Beer Lambert
0.0 2.0
200 250 300 350 400 450
Spectrophotometer
An instrument which can measure the absorbance of a
sample at any wavelength
Slits
Instrument to measures the intensity of fluorescent light emitted by a sample exposed to UV light under specific conditions.
Emit fluorescent light
as energy decreases
Ground state
Sample 90°C
Detector
UV Light Source
Monochromator Monochromator
Antibonding Antibonding Nonbonding Bonding Bonding Energy
σ π
σ π
σ −>σ
π −>π '
' '
' n->
n
σ n->π'
Electron's molecular energy levels
Fluorometer
The optics of the light source in UV-visible spectroscopy
allow either visible [approx 400nm (blue end) to 750nm
(red end) ] or ultraviolet (below 400nm) to be directed at
the sample under analysis (common range: 200 – 800 nm)
UV/Vis Spectrophotometer
Trang 5UV Spectrophotometer
Quartz (crystalline silica)
Visible Spectrophotometer
Glass, Plastic
Light Sources
UV Spectrophotometer
Visible Spectrophotometer
UV Spectrometer Application
Protein
Amino Acids (aromatic)
Pantothenic Acid
Glucose Determination
Enzyme Activity (Hexokinase)
Visible Spectrometer Application
Niacin Pyridoxine Vitamin B12 Metal Determination (Fe) Fat-quality Determination (TBA) Enzyme Activity (glucose oxidase)
Flurometric Application
Thiamin (365 nm, 435 nm)
Riboflavin
Vitamin A
Vitamin C
Standard Practice
• Prepare standards of known concentration
• Measure absorbance at λmax of solution
at different concentration
• Plot A vs concentration
• Obtain slope
• Use slope (and intercept) to determine the concentration of the analyte in the
unknown
Trang 6Typical Beer’s Law Plot
y = 0.02x
0
0.2
0.4
0.6
0.8
1
1.2
concentration (uM)
R 2 = 0.995
Characteristics of Beer’s Law Plots
• One wavelength
• Good plots have a range of absorbances from 0.010 to 1.000
• Absorbances over 1.000 are not that valid and should be avoided
Chromophoric Structure
Practice Examples
1 Calculate the Molar Extinction Coefficient E at 351 nm for aquocobalamin in 0.1 M phosphate buffer pH = 7.0 from the following data which were obtained in 1 Cm cell
2 The molar extinction coefficient (E) of compound riboflavinis 3 x 103Liter/Cm x Mole If the absorbance reading (A) at 350 nm is 0.9 using a cell of 1 Cm, what is the concentration of compound riboflavin in sample?
the absorption of the solution at 300 nm using 1 Cm quartz cell
was 0.4 What is the molar extinction coefficient of compound
Y?
4 Calculate the molar extinction coefficient E at 351 nm for
aquocobalamin in 0.1 M phosphate buffer pH =7.0 from the
following data which were obtained in 1 Cm cell
Spectroscopy Homework
1 A substance absorbs at 600 nm and 4000 nm What type of energy transition most likely accounts for each of these absorption processes?
2 Complete the following table
[X](M) = Concentration in Mole/L
Trang 7is 30,000 at 550 nm What is the absorptivity in L/g-cm.
4 The iron complex of o-phenanthroline (Molecular weight
236) has molar absorptivity of 10,000 at 525 nm If the
absorbance of 0.01 is the lowest detectable signal, what
concentration in part per million can be detected in a 1-cm
cell?