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1 Created by Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass Spectrometry Copyright © 2014 by John Wiley & Sons, Inc. All rights reserved. Classic methods for organic structure determination Require large quantities of sample and are time consuming © 2014 by John Wiley & Sons, Inc. All rights reserved.
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Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Page 1: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

1

Created byProfessor William Tam & Dr. Phillis Chang

Chapter 9

Nuclear MagneticResonance and Mass

Spectrometry

Copyright © 2014 by John Wiley & Sons, Inc. All rights reserved.

Classic methods for organic structure determination● Require large quantities of

sample and are time consuming

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 2: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Spectroscopic methods for organic structure determinationa) Mass Spectroscopy (MS)

● Molecular Mass & characteristic fragmentation pattern

b) Infrared Spectroscopy (IR)● Characteristic functional groups

c) Ultraviolet Spectroscopy (UV) ● Characteristic chromophore

d) Nuclear Magnetic Resonance (NMR)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

General steps for structure elucidation 1. Elemental analysis

● Empirical formula● e.g. C2H4O

2. Mass spectrometry● Molecular weight● Molecular formula● e.g. C4H8O2, C6H12O3 … etc.● Characteristic fragmentation

pattern for certain functional groups

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 3: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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General steps for structure elucidation 3. From molecular formula

● Double bond equivalent (DBE)

4. Infrared spectroscopy (IR)● Identify some specific

functional groups● e.g. C=O, C–O, O–H, COOH,

NH2 … etc.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

General steps for structure elucidation 5. UV (Ultraviolet) Spectroscopy

● Sometimes useful especially for conjugated systems

● e.g. dienes, aromatics, enones

6. 1H, 13C NMR and other advanced NMR techniques● Full structure determination

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 4: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Electromagnetic spectrum

cosmic & -rays

X-rays ultraviolet visible infrared micro-wave

radio-wave

1Å = 10-10m

1nm = 10-9m

1m = 10-6m

0.1nm 200nm 400nm 800nm 50m

X-RayCrystallography

UV IR NMR

© 2014 by John Wiley & Sons, Inc. All rights reserved.

2. Nuclear Magnetic Resonance(NMR) Spectroscopy

A graph that shows the characteristic energy absorption frequencies and intensities for a sample in a magnetic field is called a nuclear magnetic resonance (NMR) spectrum

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 5: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

5

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Typical 1H NMR spectrum● Chemical Shift ()

● Integration (areas of peaks no. of H)

● Multiplicity (spin-spin splitting) and coupling constant

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 6: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Typical 1H NMR spectrum

Record as: 1H NMR (300 MHz, CDCl3):

4.35 (2H, t, J = 7.2 Hz, Hc)

2.05 (2H, sextet, J = 7.2 Hz, Hb)

1.02 (3H, t, J = 7.2 Hz, Ha)

chemicalshift () in ppm

no. of H(integration) multiplicity

couplingconstantin Hz

© 2014 by John Wiley & Sons, Inc. All rights reserved.

2A. Chemical Shift The position of a signal along the x-axis of

an NMR spectrum is called its chemical shift

The chemical shift of each signal gives information about the structural environment of the nuclei producing that signal

Counting the number of signals in a 1H NMR spectrum indicates, at a first approximation, the number of distinct proton environments in a molecule

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 7: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

Normal range of 1H NMR

15 -10 ppm

"upfield" (more shielded)

"downfield" (deshielded)

(high field strength)

(low field strength)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 8: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Reference compound● TMS = tetramethylsilane

as a reference standard (0 ppm)● Reasons for the choice of TMS as

reference Resonance position at higher field

than other organic compounds Unreactive and stable, not toxic Volatile and easily removed

(B.P. = 28oC)

MeSi MeMeMe

© 2014 by John Wiley & Sons, Inc. All rights reserved.

NMR solvent● Normal NMR solvents should not

contain hydrogen● Common solvents

CDCl3 C6D6

CD3OD

CD3COCD3 (d6-acetone)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 9: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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The 300-MHz 1H NMR spectrum of 1,4-dimethylbenzene

© 2014 by John Wiley & Sons, Inc. All rights reserved.

2B. Integration of Signal Areas

Integral Step Heights The area under each signal in a 1H

NMR spectrum is proportional to the number of hydrogen atoms producing that signal

It is signal area (integration), not signal height, that gives information about the number of hydrogen atoms

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 10: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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O

Ha HaHb

HbHbR

HaHb

2 Ha 3 Hb

© 2014 by John Wiley & Sons, Inc. All rights reserved.

2C. Coupling (Signal Splitting) Coupling is caused by the magnetic

effect of nonequivalent hydrogen atoms that are within 2 or 3 bonds of the hydrogens producing the signal

The n+1 rule● Rule of Multiplicity:

If a proton (or a set of magnetically equivalent nuclei) has n neighbors of magnetically equivalent protons, its multiplicity is n + 1

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 11: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Examples

Hb C C ClHaHb

Hb Ha

Ha: multiplicity = 3 + 1 = 4 (a quartet)

Hb: multiplicity = 2 + 1 = 3 (a triplet)

(1)

Cl C C ClHbHa

Cl Hb

Ha: multiplicity = 2 + 1 = 3 (a triplet)

Hb: multiplicity = 1 + 1 = 2 (a doublet)

(2)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 12: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Examples

Note: All Hb’s are chemically and magnetically equivalent.

Hb C C BrHaHb

Hb

Ha: multiplicity = 6 + 1 = 7 (a septet)

Hb: multiplicity = 1 + 1 = 2 (a doublet)

(3)

HbHb

Hb

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Pascal’s Triangle● Use to predict relative intensity of

various peaks in multiplet● Given by the coefficient of

binomial expansion (a + b)n

singlet (s) 1doublet (d) 1 1triplet (t) 1 2 1quartet (q) 1 3 3 1quintet 1 4 6 4 1sextet 1 5 10 10 5 1

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 13: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Pascal’s Triangle

● For

● For

Br C C BrHbHa

Cl Cl

Due to symmetry, Ha

and Hb are identical a singlet

Cl C C BrHbHa

Cl Br

Ha ≠ Hb

two doublets

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Example: 1H NMR (300 MHz) of an unknown compound with molecular formula C3H7Br

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 14: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Three distinct signals at ~ 3.4, 1.8and 1.1 ppm 3.4 ppm: likely to be near an

electronegative group (Br)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

(ppm): 3.4 1.8 1.1

Integral: 2 2 3

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 15: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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(ppm): 3.4 1.8 1.1

Multiplicity: triplet sextet triplet

2 H's on adjacent C

5 H's on adjacent C

2 H's on adjacent C

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Complete structure:

BrCH2

CH2

CH3

• 2 H's from integration

• triplet

• 2 H's from integration

• sextet

• 3 H's from integration

• triplet

most upfield signalmost downfieldsignal

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 16: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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4. Nuclear Spin:The Origin of the Signal

The magnetic field associated with a spinning

proton

The spinning proton

resembles a tiny bar magnet

© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 17: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

Spin quantum number (I)

1H: I = ½ (two spin states: +½ or -½) (similar for 13C, 19F, 31P)

12C, 16O, 32S: I = 0 These nuclei do not give an NMR

spectrum

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 18: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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5. Detecting the Signal: Fourier Transform NMR Spectrometers

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 19: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 20: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 21: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 22: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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6. The Chemical Shift

© 2014 by John Wiley & Sons, Inc. All rights reserved.

The chemical shift of a proton, when expressed in hertz (Hz), is proportional to the strength of the external magnetic field

Since spectrometers with different magnetic field strengths are commonly used, it is desirable to express chemical shifts in a form that is independent of the strength of the external field

6A. PPM and the Scale

Page 23: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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For example, the chemical shift for benzene protons is 2181 Hz when the instrument is operating at 300 MHz. Therefore

The chemical shift of benzene protons in a 60 MHz instrument is 436 Hz:

Thus, the chemical shift expressed in ppm is the same whether measured with an instrument operating at 300 or 60 MHz (or any other field strength)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 24: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

Protons absorb at different NMR frequencies depending on the electron density around them and the effects of local induced magnetic fields

All protons do not absorb energy at the same frequency in a given external magnetic field

Lower chemical shift values correspond with lower frequency

Higher chemical shift values correspond with higher frequency

7. Shielding & Deshielding of Protons

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 25: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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15 -10 ppm

"upfield" (more shielded)

"downfield" (deshielded)

(high field strength)

(low field strength)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 26: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 27: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Protons of Hydrogen Atoms in AlkylC–H Groups● The chemical shift for hydrogens of

unsubstituted alkanes is typically in the range of 0.8–1.8

Protons of Hydrogens Near Electro-negative Groups● The chemical shift of hydrogens bonded

to a carbon bearing oxygen or a halogen is typically in the range of 3.1–4.0

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 28: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Deshielding by electronegative groups

CH3X

X = F OH Cl Br I H

Electro-negativity 4.0 3.5 3.1 2.8 2.5 2.1

(ppm) 4.26 3.40 3.05 2.68 2.16 0.23

● Greater electronegativity Deshielding of the proton Larger

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Electronegativity

Page 29: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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● If we were to consider only the relative electronegativities of carbon in its three hybridization states, we might expect the following order of protons attached to each type of carbon:

(higher frequency) sp < sp2 < sp3 (lower

frequency)© 2014 by John Wiley & Sons, Inc. All rights reserved.

● In fact, protons of terminal alkynes absorb between 2.0 and 3.0, and the order is

(higher frequency)

sp2 < sp < sp3 (lower frequency)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 30: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

Shielding and deshielding by circulation of electrons

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 31: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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● e.g.

Hd Hc

Hb

Ha

(ppm)Ha & Hb: 7.9 & 7.4 (deshielded)Hc & Hd: 0.91 – 1.2 (shielded)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

● Aldehydes

OR

H

Electronegativity effect + Anisotropy effect = 8.5 – 10 ppm (deshielded)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 32: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Two or more protons that are in identical environments have the same chemical shift and, therefore, give only one 1H NMR signal

Chemically equivalent protons are chemical shift equivalent in 1H NMR spectra

8. Chemical Shift Equivalent and Nonequivalent Protons

© 2014 by John Wiley & Sons, Inc. All rights reserved.

8A. Homotopic and Heterotopic Atoms If replacing the hydrogens by a

different atom gives the same compound, the hydrogens are said to be homotopic

Homotopic hydrogens have identical environments and will have the same chemical shift. They are said to be chemical shift equivalent

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 33: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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HC CHH

HH

H

Ethane

HC CHH

HH

Br

HC CHH

BrH

H

HC CHH

HBr

HHCC HH

HBr

H

HCC HH

BrH

H

HCC HH

HH

Br

The six hydrogens of ethane are homotopicand are, therefore, chemical shift equivalent

Ethane, consequently, gives only one signal in its 1H NMR spectrum

sam

e co

mpo

unds

same com

pounds

© 2014 by John Wiley & Sons, Inc. All rights reserved.

If replacing hydrogens by a different atom gives different compounds, the hydrogens are said to be heterotopic

Heterotopic atoms have different chemical shifts and are not chemical shift equivalent

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 34: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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HC CHH

HH

Br

HC CHH

HCl

BrBrCC HH

HCl

H

BrCC HH

HCl

H

BrCC HH

ClH

H

BrCC HH

HH

Cl

These 2 H’s are also homotopic to each other

different compounds heterotopic

same compounds these 3 H’s of the CH3 group are homotopic the CH3group gives only one 1H NMR signal

© 2014 by John Wiley & Sons, Inc. All rights reserved.

HC CHH

HH

Br

CH3CH2Br● two sets of hydrogens that are

heterotopic with respect to each other

● two 1H NMR signals

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 35: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Other examples

(1) C CH

H

CH3

CH3 2 1H NMR signals

(2) H

CH3H

H

H CH3

4 1H NMR signals

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Other examples

(3) H3CCH3

H H

H

H

H H

3 1H NMR signals

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 36: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

36

Application to 13C NMR spectroscopy● Examples

(1) H3C CH3 1 13C NMR signal

(2)

CH3

CH3 4 13C NMR signals

© 2014 by John Wiley & Sons, Inc. All rights reserved.

(3)

OHHO

5 13C NMR signals

(4)HO

HO 4 13C NMR signals

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 37: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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8B. Enantiotopic and Diastereotopic Hydrogen Atoms

If replacement of each of two hydrogen atoms by the same group yields compounds that are enantiomers, the two hydrogen atoms are said to be enantiotopic

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Enantiotopic hydrogen atoms have the same chemical shift and give only one 1H NMR signal:

H3C Br

H H

H3C Br

H G

H3C Br

G H

enantiomer

enantiotopic

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 38: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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CH3

H OHH3C

HaHb

dias

tere

omer

s

diastereotopic

CH3

H OHH3C

GHb

CH3

H OHH3C

HaG

chiralitycenter

© 2014 by John Wiley & Sons, Inc. All rights reserved.

HbBrHa

H

dias

tere

omer

s

diastereotopic

HbBrG

H

GBr

Ha

H

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 39: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

Vicinal coupling is coupling between hydrogen atoms on adjacent carbons (vicinal hydrogens), where separation between the hydrogens is by three bonds

9. Signal Splitting:Spin–Spin Coupling

Ha Hb3J or vicinal coupling

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 40: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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9A. Vicinal Coupling Vicinal coupling between heterotopic

protons generally follows the n + 1 rule. Exceptions to the n + 1 rule can occur when diastereotopic hydrogens or conformationally restricted systems are involved

Signal splitting is not observed for protons that are homotopic(chemical shift equivalent) or enantiotopic

© 2014 by John Wiley & Sons, Inc. All rights reserved.

9B. Splitting Tree Diagrams and the Origin of Signal Splitting

Splitting analysis for a doublet

C CHaHb

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 41: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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C C

H H

C C

H HA A

upfielddownfield

Bo

THE CHEMICAL SHIFT OF PROTON HA IS AFFECTED BY THE SPIN OF ITS NEIGHBORS

50 % ofmolecules

50 % ofmolecules

At any given time about half of the molecules in solution willhave spin +1/2 and the other half will have spin -1/2.

aligned with Bo opposed to Bo

neighbor aligned neighbor opposed

+1/2 -1/2

Page 42: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Splitting analysis for a triplet

CHb

CHaHb

C C CHaHb Hb

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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43

Splitting analysis for a quartet

Hb CHb

CHaHb

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Pascal’s Triangle● Use to predict relative intensity of

various peaks in multiplet● Given by the coefficient of

binomial expansion (a + b)n

singlet (s) 1doublet (d) 1 1triplet (t) 1 2 1quartet (q) 1 3 3 1quintet 1 4 6 4 1sextet 1 5 10 10 5 1

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 44: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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9C. Coupling Constants – Recognizing Splitting Patterns

X CHa

CHb

HbHbHa

© 2014 by John Wiley & Sons, Inc. All rights reserved.

9D. The Dependence of Coupling Constants on Dihedral Angle

3J values are related to the dihedral angle ()

H

H

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 45: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Karplus curve

~0o or 180o

Maximum 3J value

~90o

3J ~0 Hz

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Karplus curve● Examples

Hb

Ha

Hb

Ha

= 180º

Ja,b = 10-14 Hz

(axial, axial)

Hb

Ha

Hb

Ha

= 60º

Ja,b = 4-5 Hz

(equatorial, equatorial)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 46: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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Karplus curve● Examples

Hb

Ha

Hb

Ha

= 60º

Ja,b = 4-5 Hz

(equatorial, axial)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

9E. Complicating Features The 60 MHz 1H NMR spectrum of ethyl

chloroacetate

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 47: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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The 300 MHz 1H NMR spectrum of ethyl chloroacetate

© 2014 by John Wiley & Sons, Inc. All rights reserved.

9F. Analysis of Complex Interactions

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Page 48: Nuclear Magnetic Resonance and Mass Spectrometryhome.konkuk.ac.kr/~parkyong/Classes/ch9.pdf · Professor William Tam & Dr. Phillis Chang Chapter 9 Nuclear Magnetic Resonance and Mass

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The 300 MHz 1H NMR spectrum of1-nitropropane

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Protons of alcohols (ROH) and amines (RNH2) may appear over a wide range from 0.5 – 5.0 ppm● Hydrogen-bonding is the reason for this

range

10. Proton NMR Spectra and Rate Processes

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Why don’t we see coupling with the O–H proton, e.g. –CH2–OH (triplet?)

● Because the acidic protons are exchangeable about 105 protons per second (residence time 10-5 sec), but the NMR experiment requires a time of 10-2 – 10-3 sec. to “take” a spectrum, usually we just see an average. Thus, OH protons are usually a broad singlet.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

+ 50 °C

- 30 °C

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Deuterium Exchange

● To determine which signal in the NMR spectrum is the OH proton, shake the NMR sample with a drop of D2O and whichever peak disappears that is the OH peak (note: a new peak of HOD appears)

D2O + HODR O H R O D

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Phenols● Phenol protons appear downfield at

4-7 ppm● They are more “acidic” - more H+

character● More dilute solutions - peak

appears upfield: towards 4 ppm

OH O H

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Phenols● Intramolecular H-bonding causes

downfield shift

OH

O12.1 ppm

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

Unlike 1H with natural abundance ~99.98%, only 1.1% of carbon, namely 13C, is NMR active

11. Carbon-13 NMR Spectroscopy11A. Interpretation of 13C NMR

Spectra

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11B. One Peak for Each Magnetically Distinct Carbon Atom

13C NMR spectra have only become commonplace more recently with the introduction of the Fourier Transform (FT) technique, where averaging of many scans is possible (note 13C spectra are 6000 times weaker than 1H spectra, thus requiring a lot more scans for a good spectrum)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Note for a 200 MHz NMR (field strength 4.70 Tesla)

● 1H NMR Frequency = 200 MHz

● 13C NMR Frequency = 50 MHz

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12C is not NMR-active I = 0

however…. 13C does have spin, I = 1/2 (odd mass)

1. Natural abundance of 13C is small (1.08% of all C)

2. Magnetic moment of 13C is small

13C signals are weaker than 1H because:

13C NMR

PULSED FT-NMR IS REQUIRED

The chemical shift range is larger than for protons

0 - 200 ppm

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13C NMR

For a given field strength 13C has its resonance at adifferent (lower) frequency than 1H.

1H

13C1.41 T 60 MHz2.35 T 100 MHz7.05 T 300 MHz

1.41 T 15.1 MHz2.35 T 25.0 MHz7.05 T 75.0 MHz

Divide the hydrogenfrequency by 4 (approximately)

for carbon-13

CH3 C CH2 CH3

H

OH

Example:● 2-Butanol

Proton-coupled13C NMR spectrum

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CH3 C CH2 CH3

H

OH

Example:● 2-Butanol

Proton-decoupled13C NMR spectrum

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AldehydesKetones

Acids AmidesEsters Anhydrides

Aromatic ringcarbons

Unsaturated carbon - sp2

Alkyne carbons - sp

Saturated carbon - sp3

electronegativity effects

Saturated carbon - sp3

no electronegativity effects

C=O

C=O

C=CC C

200 150 100 50 0

200 150 100 50 0

8 - 30

15 - 55

20 - 60

40 - 80

35 - 80

25 - 65

65 - 90

100 - 150

110 - 175

155 - 185

185 - 220

Correlation chart for 13C Chemical Shifts (ppm)

C-O

C-Cl

C-Br

R3CH R4C

R-CH2-R

R-CH3

RANGE

/

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11C. 13C Chemical Shifts Decreased electron density around an

atom deshields the atom from the magnetic field and causes its signal to occur further downfield (higher ppm, to the left) in the NMR spectrum

Relatively higher electron density around an atom shields the atom from the magnetic field and causes the signal to occur upfield (lower ppm, to the right) in the NMR spectrum

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Electronegative substituents cause downfield shift

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

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Hybridization of carbon

● sp2 > sp > sp3

H2C CH2 HC CH H3C CH3

e.g.

123.3 ppm 71.9 ppm 5.7 ppm

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Anisotropy effect

● Shows shifts similar to the effect in 1H NMR

C C

e.g.

C

shows largeupfield shift

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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BROMOCYCLOHEXANE

Cl CH2 CH CH3

OH

(a) (b) (c)

1-Chloro-2-propanol

(a)(b)

(c)

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Cl

Cla

a

b

b

c

c

1,2-DICHLOROBENZENE

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Because of its low natural abundance (0.0108) thereis a low probability of finding two 13C atoms next toeach other in a single molecule.

However, 13C does couple to hydrogen atoms (I = 1/2)

13C - 13C coupling NO!

13C - 1H coupling YES!

Spectra are determined by many molecules contributingto the spectrum, each having only one 13C atom.

13C NMR (cont)

not probable

very common

Homonuclear: Spin-spin splitting patterns where the interaction occurs between two

atoms that are of the same type of nucleus.

3JH-H = 1-20 Hz

Heteronuclear: Spin-spin splitting patterns where the interaction occurs between two atoms that are of different types of nuclei.

1JC-H = 100-250 Hz

Spin-Spin Coupling (scalar)

H

C C

H

H

C C

H

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The effect of attached protons on 13C resonances

n+1 = 4 n+1 = 3 n+1 = 2 n+1 = 1

C13

3 protons 2 protons 1 proton 0 protons

H

H

H

C13

H

H

C13

H C13

Methylcarbon

Methylenecarbon

Methinecarbon

Quaternarycarbon

( n+1 rule applies )

COUPLING TO ATTACHED PROTONS

(J’s are large ~ 100 - 200 Hz)

ETHYL PHENYLACETATE

13C coupledto the hydrogens

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ETHYL PHENYLACETATE

13C coupledto the hydrogens

13C decoupledfrom the hydrogens

in some casesthe peaks of the multiplets willoverlap

this is aneasier spectrumto interpret

The NMR Spectrum - 13C

1H Coupled (undecoupled)

1H Decoupled

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The broadband proton-decoupled 13C NMR spectrum of methyl methacrylate

© 2014 by John Wiley & Sons, Inc. All rights reserved.

11D. DEPT 13C Spectra DEPT 13C NMR spectra indicate how

many hydrogen atoms are bonded to each carbon, while also providing the chemical shift information contained in a broadband proton-decoupled 13C NMR spectrum. The carbon signals in a DEPT spectrum are classified as CH3, CH2, CH, or C accordingly

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Cl CH2 CH CH3

OH

(a) (b) (c)

1-Chloro-2-propanol

(a)(b) (c)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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HCOSY● 1H–1H correlation spectroscopy

HETCOR● Heteronuclear correlation

spectroscopy

12. Two-Dimensional (2D) NMR Techniques

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12A. 1H–1H COSY Cross-Peak Correlations

HCOSY of 2-chloro-butane

H2

H1

H1

H3

H3

H4

H4

H2

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12B. 1H–13C Heteronuclear Corre-lationCross-Peak Correlations

HETCOR of 2-chloro-butane

H1

H2

H3

H4

C1

C2

C3 C

4

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

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In the mass spectrometer, a molecule in the gaseous phase under low pressure is bombarded with a beam of high-energy electrons (70 eV or ~ 1600 kcal/mol)

This beam can dislodge an electron from a molecule to give a radical cation which is called the molecular ion, M+ or more accurately

14. Formation of Ions: Electron Impact Ionization

M70 eV e-

M© 2014 by John Wiley & Sons, Inc. All rights reserved.

EI

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The M+ peak at 114 is referred to as the parent peak or molecular ion

C8H18e-

70 eV+ 2 e-[C8H18]

(M+)

The largest or most abundant peak is called the base peak and is assigned an intensity of 100%, other peaks are then fractions of that e.g. 114(M+,40), 85(80), 71(60), 57(100) etc.

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Partial MS of octane (C8H18, M = 114)

13. An Introduction to Mass Spectrometry

114

85

71

57M+

29 (CH3CH2)

14 (CH2)

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Masses are usually rounded off to whole numbers assuming:H = 1, C = 12, N = 14, O = 16, F = 19 etc.

Molecular ion (parent peak)

Daughterions

[C8H18]

(M+, 114)

[C6H13]

(85)

fragmentation

-CH3CH2 (29)

[C5H11]

(71)-CH3CH2CH2 (29+14)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Fragmentation

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15. Depicting the Molecular Ion

CH3CH2 CH3

H3C OH H3C N CH3

CH3

H2C CHCH2CH3

Methanol Trimethylamine 1-Butene

Radical cations from ionizationof nonbonding on electron

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CompoundIonization

Potential (eV)CH3(CH2)3NH2 8.7C6H6 (benzene) 9.2C2H4 10.5CH3OH 10.8C2H6 11.5CH4 12.7

Ionization potentials of selected molecules

© 2014 by John Wiley & Sons, Inc. All rights reserved.

16A. Fragmentation by Cleavage at a Single Bond

When a molecular ion fragments, it will yield a neutral radical (not detected) and a carbocation (detected) with an even number of electrons

The fragmentation will be dictated to some extent by the fragmentation of the more stable carbocation:ArCH2

+ > CH2=CHCH2+ > 3o > 2o > 1o > CH3

+

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e.g.

R CH

R+ CH3+

R +CH3+X

● Site of ionization: n > >

non-bonding

© 2014 by John Wiley & Sons, Inc. All rights reserved.

As the carbon skeleton becomes more highly branched, the intensity of the molecular ion peak decreases

Butane vs. isobutane

70eVe-

M+(58)

70eVe-

M+(58)

aCH3+

(43)a

b CH2CH3+(29)

b

CH3+(43)

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16B. Fragmentation of Longer Chain and Branched Alkanes

Octane vs. isooctane

M+(114)

(85)

(71)

(57)

(43)

M+(114)

+

+

+

+

+(57)

© 2014 by John Wiley & Sons, Inc. All rights reserved.

2,2,4-trimethylpentane

• Branched alkanes have small or absent M+

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16C. Fragmentation to Form Resonance-Stabilized Cations

Alkenes● Important fragmentation of terminal

alkenes Allyl carbocation (m/e = 41)

R

(41)

R +

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Alkene Fragmentation– Fairly prominent M+

– Fragment ions of CnH2n+ and CnH2n-1+

– Terminal alkenes lose allyl cation if possible to form resonance-stabilized allylic cations

R - R

[CH2=CHCH2 CH2 CH3 ] CH2 =CHCH2+ + • CH2 CH3

+•

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Carbon–carbon bonds next to an atom with an unshared electron pair usually break readily because the resulting carbocation is resonance stabilized

Ethers● Cleavage (to ether oxygen) C–C bonds

O

O

(m/e = 59)

+ OCH3

© 2014 by John Wiley & Sons, Inc. All rights reserved.

n-butyl ether

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Alcohols● Most common fragmentation: loss of

alkyl groups

OH

M+(74)

a

OH OHCH3CH2 +

b

(m/e = 45)

b

© 2014 by John Wiley & Sons, Inc. All rights reserved.

2-pentanol

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3-methyl-2-butanol

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Hydrogen atom transfer

Aldehydes● M+ peak usually observed but may

be fairly weak

● Common fragmentation pattern -cleavage

RR H

OH C OR

C OH

+

+(m/e = 29)

acylium ion

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hexanal

Ketones● -cleavage

O a

a

b

b

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Aromatic hydrocarbons● very intense M+ peaks ● characteristic fragmentation pattern

(when an alkyl group attached to the benzene ring): tropylium cation

CH3CH2

CH3

(m/e = 91)tropylium cation

rearrangement+

benzyl cation

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Benzene derivatives produce a variety of resonance stabilized ions.

CH2CH2CH2CH3 CH2CH2 CH2 CH2

CH2

m/e = 91

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+

+

Tropylium ion

16D. Fragmentation by Cleavage of Two Bonds

Alcohols frequently show a prominent peak at M - 18. This corresponds to the loss of a molecule of water

● May lose H2O by 1,2- or 1,4-elimination

+●

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1,2-elimination:OH

+ H2O

M (M - 18)

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1,4-elimination

2-pentanol

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Cycloalkenes show a characteristic fragmentation pattern which corresponds to a reverse Diels-Alder reaction

e.g.

retro Diels-Alder+

+

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H

CH2

H

H(m/e = 92)

+

McLafferty Rearrangement

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Mc Lafferty Rearrangement

Mc Lafferty Rearrangement

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Ketones● McLafferty rearrangement

O

HOH OH

OHOH

OH

+

(m/e = 86)

(m/e = 58)

+

1st McL. Rearr.

2nd McL. Rearr.

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2-octanone displays both cleavage and McLafferty

CH3CO+

resulting from cleavage.

CH3CH2CH2CH2CH2CH2CO+

resulting from cleavage.

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OH H

OH OH

(m/e = 86)2º radical

observedi

i

OH

1º radical

OH

(m/e = 114)NOT observed

ii

ii

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Characteristics of McLaffertyrearrangements1. No alkyl migrations to C=O, only H

migrates

OH

O

O

R

R

R

H

HX

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Characteristics of McLaffertyrearrangements2. 2o is preferred over 1o

OH H

iiiOH

2º radical

OH

1º radical

not

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17. Isotopes in Mass Spectra

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13C and 12CAbout 1.1% of all carbon atoms are the 13C isotope

About 98.9% of the methane molecules in the sample will contain 12C, and the other 1.1% will contain 13C

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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102

Example● Consider 100 molecules of CH4

M : 16

H1

C12H1 H1

H1

H1

C13H1 H1

H1

H1

C12H1 H2

H1

M + 1 = 17

C12: 100 C13: 1.11

H1: 100 H2: 0.016© 2014 by John Wiley & Sons, Inc. All rights reserved.

M : 16

H1

C12H1 H1

H1

H1

C13H1 H1

H1

H1

C12H1 H2

H1

M + 1 = 17

1.11 molecules contain a 13C atom

4x0.016 = 0.064 molecules contain a 2H atom

Intensity of M + 1 peak:1.11+0.064=1.174% of the M peak

+●

+●

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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100

1.17m/z

rela

tive

ion

abun

danc

eM

M +1

+●

+●

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

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© 2014 by John Wiley & Sons, Inc. All rights reserved.

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Example 1

● O2, N2H4 and CH3OH all have M.W. of 32 (by MS), but accurate masses are different O2 = 2(15.9949) = 31.9898

N2H4 = 2(14.0031) + 4(1.00783) = 32.0375

CH4O = 12.00000 + 4(1.00783) + 15.9949 = 32.0262

© 2014 by John Wiley & Sons, Inc. All rights reserved.

Example 2

● Both C3H8O and C2H4O2 have M.W. of 60 (by MS), but accurate masses are different

C3H8O = 60.05754

C2H4O2 = 60.02112

© 2014 by John Wiley & Sons, Inc. All rights reserved.

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Low Resolution Mass

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High Resolution Mass

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Identify which one of the following isomers of C6H14 has the C-13 NMR below.

A) CH3CH2CH2CH2CH2CH3 C) (CH3)2CHCH(CH3)2

B) CH3CH2CH2CH(CH3)2 D) CH3CH2C(CH3)3

A) CH3CH2CH2CH2CH2CH3 C) (CH3)2CHCH(CH3)2 B) CH3CH2CH2CH(CH3)2 D) CH3CH2C(CH3)3

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m/e = 72 ?

72

O