MCAT Organic Chemistry - Spectroscopy

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39 Terms

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Spectroscopy

measures the energy differences between the possible states of a molecular system by determining the frequencies of electromagnetic radiation absorbed by the molecules

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<p>magnetic resonance imaging (MRI)</p>

magnetic resonance imaging (MRI)

measure 1Hā€“NMR spectra of water molecules in different environments in the body; multiple cross-sectional scans of the patientā€™s body are taken, and the various chemical shifts of absorbing protons are translated into specific shades of grey which produces a picture that shows the relative density of specific types of protons

dark area = waters

light area = fattier tissue

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Infrared (IR) spectroscopy

measures molecular vibrations, which helps estimate types of bonds; infrared light is passed through a sample, and the absorbance is measured; for an absorption to be recorded, the vibration must result in a change in the bond dipole moment

range: 2500 to 25,000 nm = 4000 to 400 cmāˆ’1

<p>measures molecular vibrations, which helps estimate types of bonds; infrared light is passed through a sample, and the absorbance is measured; for an absorption to be recorded, the vibration must result in a change in the bond dipole moment</p><p>range: 2500 to 25,000 nm = 4000 to 400 cm<sup>āˆ’1</sup></p>
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infrared light range

700 nm to 1 mm

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wavenumber

analog of frequency

= 1/Ī»

units: cmāˆ’1

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molecular vibration

bond stretching, bending, or combinations of different vibrational modes; include twisting and folding; Symmetric stretches do not show up in IR spectra because they involve no net change in dipole movement

<p>bond stretching, bending, or combinations of different vibrational modes; include twisting and folding; Symmetric stretches do not show up in IR spectra because they involve no net change in dipole movement</p>
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fingerprint region

complex vibration patterns, caused by the motion of the molecule as a whole, in the 1500 to 400 cmāˆ’1 range; the specific absorbance pattern is characteristic of each individual molecule

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hydroxyl group (Oāˆ’H) IR

broad (wide) peak

3300 cmāˆ’1 for alcohols

3000 cmāˆ’1 for carboxylic acids (carbonyl pulls electron density ā†’ shifts absorption lower)

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carbonyl group (C=O) IR

sharp (deep) peak

around 1700 cmāˆ’1

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amine group (Nāˆ’H) IR

same region as Oāˆ’H bonds, but have a sharp peak

around 3300 cmāˆ’1

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transmittance

the amount of light that passes through the sample and reaches the detector

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IR spectra

plotted as percent transmittance vs. wavenumber; maximum absorptions appear as the bottoms of valleys on the spectrum

<p>plotted as percent transmittance vs. wavenumber; maximum absorptions appear as the bottoms of valleys on the spectrum</p>
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ultraviolet-visible (UV-vis) spectroscopy

passing ultraviolet light through a sample that is usually dissolved in an inert, nonabsorbing solvent, and recording the absorbance, caused by electronic transitions between orbitals; wavelength of maximum absorbance, which tells us the extent of conjugation within conjugated systems

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UV spectra

plots absorbance vs. wavelength

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HOMOā€“LUMO gap

energy gap between highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO); lower energy gap = longer wavelengths = more conjugation = more excitable

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Conjugation

molecules with unhybridized p-orbitals, can be excited by ultraviolet light; shifting the absorption spectrum, resulting in higher maximum wavelengths; larger conjugated molecules may even absorb light in the visible range ā†’ coloured compounds

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Nuclear magnetic resonance (NMR)

certain atomic nuclei have magnetic moments that tend to align either with or against the direction of an applied field; irradiated with radiofrequency pulses that match the energy gap between the two states, exciting some nuclei depending on an atomā€™s magnetic environment

<p>certain atomic nuclei have magnetic moments that tend to align either with or against the direction of an applied field; irradiated with radiofrequency pulses that match the energy gap between the two states, exciting some nuclei depending on an atomā€™s magnetic environment</p>
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Ī±-state

Nuclei with magnetic moments that are aligned with the magnetic field; lower energy

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Ī²-state

Nuclei with magnetic moments that are aligned against the magnetic field; higher energy

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chemical shift (Ī“)

standardized method of plotting the NMR spectrum using an arbitrary variable with units of parts per million (ppm) of spectrometer frequency

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NMR spectra

plot of frequency vs. absorption of energy

<p>plot of frequency vs. absorption of energy</p>
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downfield

towards a larger chemical shift; increases to the left; signals become relatively deshielded

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tetramethylsilane (TMS)

calibration standard/reference peak to mark 0 ppm

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chemically equivalent

protons that have the same magnetic environment; lead to the same peak

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integration

the area under the peaks; the ratio of different peaks corresponds exactly to the ratio of protons that produced each peak

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deshielding

electron density away from the proton, leaving it more vulnerable to the magnetic field

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spinā€“spin coupling (splitting)

two protons in such close proximity to each other that are not magnetically identical; the magnetic environment of one group of protons can be affected by another

<p>two protons in such close proximity to each other that are not magnetically identical; the magnetic environment of one group of protons can be affected by another</p>
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n + 1 rule

if a proton has n protons that are three bonds away, it will be split into n + 1 peaks

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coupling constant (J)

magnitude of this splitting, measured in hertz

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multiplet

peaks that have more than four splits

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methyl group (-CH3) 1H-NMR

0.9 ppm

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methylene group (-CH1) 1H-NMR

1.25 ppm

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methine gorup (-CH) 1H-NMR

1.5 ppm

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aldehyde ((C=O)-H) 1H-NMR

9 - 10 ppm

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carboxylic acid ((C=O)-OH) 1H-NMR

10.5 - 12 ppm

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aromatic hydrogen (Ar-H) 1H-NMR

6.0 - 8.5 ppm

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sp3 hybridized carbons 1H-NMR

0.0 to 3.0 ppm

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sp2 hybridised carbons 1H-NMR

4.6 - 6.0 ppm

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sp hybridised carbon 1H-NMR

2.0 - 3.0 ppm