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SPECTROSCOPY. Light interacting with matter as an analytical tool

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SPECTROSCOPY

Light interacting with matter as an analytical tool

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X-ray: core electron excitation UV: valance electronic excitation IR: molecular vibrations Radio waves:

Nuclear spin states (in a magnetic field)

(3)

3-D structure X-rays

X-ray Crystallography

inner electrons, elemental X-rays

X-Ray Spectroscopy

nuclear spin states Radio waves FT-NMR vibrations IR/UV Raman vibrations, rotations IR/Microwave FT-IR

atomic transitions (val. e-) UV-vis region

Atomic Absorption

bonding electrons UV-vis region

UV-vis

Spectroscopic Techniques and Chemistry they Probe

(4)

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

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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

(6)

Spectroscopies

in the UV-Vis region

• UV-vis (molecular) absorption spectroscopy

• Solvated metal complexes • Molecular fluorescence

• Atomic absorption • Atomic Emission

(7)

UV-vis (molecular) absorption

spectroscopy

• Quantitative/Beer’s Law

• Valence electronic transitions • Molecular orbital theory

• Effect of conjugation

• Broadness of the spectra (solvent effect

and superimposition of vibrational/rotational levels)

• Instrumentation

• Molecular Probes/biokits based on visible absorption spectroscopy

(8)

Quantitative Spectroscopy

• Beer’s Law Aλ1 = eλ1bc

e is molar absorptivity (unique for a given compound at λ1)

b is path length c concentration

(9)

Beer’s Law

• A = -logT = log(P0/P) = ebc • T = Psolution/Psolvent = P/P0

cuvette source

slit

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• A = -logT = log(P0/P) = ebc

– e is molar absorptivity (L/mol⋅cm) – B is the path length (cm)

– T is the transmittance – T = Psolution/Psolvent = P/P0

• Works for monochromatic light

• Compound x has a unique e at different wavelengths

(11)

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

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Standard Practice

• Prepare standards of known concentration

• Measure absorbance at λmax • Plot A vs. concentration

• Obtain slope

• Use slope (and intercept) to determine the concentration of the analyte in the unknown

(13)

Typical Beer’s Law Plot

y = 0.02x 0 0.2 0.4 0.6 0.8 1 1.2 0.0 20.0 40.0 60.0 concentration (uM) A

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UV-Vis Spectroscopy

• UV- organic molecules

– Outer electron bonding transitions – conjugation

• Visible – metal/ligands in solution

– d-orbital transitions

– Dyes – very high level of conjugation

(15)

Characteristics of UV-Vis spectra of

Organic Molecules

• Absorb mostly in UV unless highly conjugated

• Spectra are broad, usually to broad for qualitative identification purposes

• Excellent for quantitative Beer’s Law-type analyses

• The most common detector for an HPLC

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Molecules have quantized energy levels: ex. electronic energy levels.

energy

hv

energy

}

ΔΕ

= hv

Q: Where do these quantized energy levels come from?

A: The electronic configurations associated with bonding.

Each electronic energy level (configuration) has

associated with it the many vibrational energy levels we examined with IR.

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Broad spectra

• Overlapping vibrational and rotational peaks

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Molecular Orbital Theory

(19)

2s 2s σ σ∗ σ σ∗ π∗ π 2p 2p

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C C

σ

σ∗

hv

σ

σ∗

σ

σ∗

C C H H H H H H

λmax = 135 nm (a high energy transition)

Absorptions having λmax < 200 nm are difficult to observe because everything (including quartz glass and air) absorbs in this spectral region.

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C C

σ

σ∗

hv

π

π∗

σ

σ∗

π

π∗

π

π∗

Example: ethylene absorbs at longer wavelengths: λmax = 165 nm ε= 10,000

ΔΕ= hv

(22)

σ

σ∗

hv

π

π∗

n

σ

σ∗

π

π∗

n C O

π∗

n

The n to pi* transition is at even lower wavelengths but is not as strong as pi to pi* transitions. It is said to be “forbidden.” Example:

Acetone: n−σ∗ λmax = 188 nm ; ε= 1860 n−π∗ λmax = 279 nm ; ε= 15

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C C C C C O C O H σ −> σ∗ 135 nm π −> π∗ 165 nm n −> σ∗ 183 nm weak π −> π∗ 150 nm n −> σ∗ 188 nm n −> π∗ 279 nm weak λ A 180 nm 279 nm C O

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C C

HOMO LUMO

Conjugated systems:

Preferred transition is between Highest Occupied Molecular Orbital (HOMO) and Lowest Unoccupied Molecular Orbital (LUMO).

Note: Additional conjugation (double bonds) lowers the HOMO-LUMO energy gap:

Example:

1,3 butadiene: λmax = 217 nm ; ε= 21,000 1,3,5-hexatriene λmax = 258 nm ; ε= 35,000

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O

O

O

Similar structures have similar UV spectra:

(26)

Lycopene:

λmax = 114 + 5(8) + 11*(48.0-1.7*11) = 476 nm λmax(Actual) = 474.

(27)
(28)

Yellow food coloring

Tartrazine

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Blue food coloring

Brilliant Blue

(30)

Solvated Metal Ions

• The Spatial arrangements of ligands around a solvated metal ion causes distortion of the d-orbital

• Consequence: d-orbital splitting

• The ΔE is often in the visible range of the spectrum

(31)

Co2+ H2O H2O H2O H2O H2O H2O

Octahedral Geometry

(32)

d-orbital splitting

Degenerate D-orbitals of naked Co d-orbitals of hydrated Co2+ Octahedral Configuration ΔE = hc/λ Max. absorbs around 490 nm, solution appears pale pink

(33)

Molecular Probes or TAGs

• Chemical reagents that have a detectable handle that can selectively bind to analyte • Example/ BCA Total protein assay

– combines reduction of Cu2+ to Cu+ by protein in an

alkaline medium with the highly sensitive and selective colorimetric detection of the cuprous cation (Cu+) by bicinchoninic acid

– Biuret rxn; chelation complex between amino groups and Cu+ (light blue)

– Cu+/BCA forms a purple complex, intense

absorption at 562 nm – Microplate reader

(34)

Instrumentation

• Fixed wavelength instruments • Scanning instruments

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Fixed Wavelength Instrument

• LED serve as source

• Pseudo-monochromatic light source

• No monochrometer necessary/ wavelength selection occurs by turning on the appropriate LED

• 4 LEDs to choose from

photodyode sample

beam of light LEDs

(36)

Scanning Instrument

cuvette Tungsten Filament (vis) slit Photomultiplier tube monochromator Deuterium lamp Filament (UV) slit Scanning Instrument

(37)

sources

• Tungten lamp (350-2500 nm) • Deuterium (200-400 nm)

(38)

Monochromator

• Braggs law, nλ = d(sin i + sin r)

• Angular dispersion, dr/dλ = n / d(cos r)

• Resolution, R = λ/Δλ = nN, resolution is extended by concave mirrors to refocus the divergent beam at the exit slit

(39)

Sample holder

• Visible; can be plastic or glass • UV; you must use quartz

(40)

Single beam vs. double beam

(41)

Diode array Instrument

cuvette Tungsten

Filament (vis)

slit

Diode array detector 328 individual detectors monochromator Deuterium lamp Filament (UV) slit mirror

(42)

Advantages/disadvantages

• Scanning instrument

– High spectral resolution (63000), λ/Δλ – Long data acquisition time (several

minutes)

– Low throughput

• Diode array

– Fast acquisition time (a couple of seconds), compatible with on-line separations

– High throughput (no slits) – Low resolution (2 nm)

(43)

High Performance Liquid

Chromatography (HPLC)

• Separation of mixtures

• Because UV-VIS spectra are so broad, components of a mixture need to be

separated prior to detection

• Marriage between HPLC and UV/vis detector – HPLC separates components

– Each component can be detected and quantified by UV-VIS detector

(44)

HPLC-UV

Mobile phase HPLC Pump syringe 6-port valve Sample loop HPLC column UV detector Solvent waste

References

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