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Lecture 37 Nuclear magnetic resonance Lecture 37 Nuclear magnetic resonance

Lecture 37 Nuclear magnetic resonance - PowerPoint Presentation

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Lecture 37 Nuclear magnetic resonance - PPT Presentation

Nuclear magnetic resonance The use of NMR in chemical research was pioneered by Herbert S Gutowski of Department of Chemistry University of Illinois who established the relationship between chemical shifts and molecular structures He also discovered spinspin coupling ID: 929579

coupling spin field magnetic spin coupling magnetic field chemical nmr group peaks hyperfine resonance constant structure shifts energy proton

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Slide1

Lecture 37

Nuclear magnetic resonance

Slide2

Nuclear magnetic resonance

The use of NMR in chemical research was pioneered by

Herbert S. Gutowski of Department of Chemistry, University of Illinois, who established the relationship between chemical shifts and molecular structures. He also discovered spin-spin coupling.Foundation of magnetic spectroscopy.Proton NMR.

Slide3

Circular electric current = magnet

Electrons in

p

,

d, f

orbitals

Electron spinNuclear spin

angular

momentum

charge

magnetic

moment

mass

Slide4

Magnet-magnetic-field interaction

high energy

low energy

Classical

Magnetic moment

Magnetic field

Quantum

Slide5

Tesla

Nikola Tesla

Public domain image from Wikipedia

kgm

2

/s

C

J

kg

T (Tesla)

1 T = 1 V s / m

2

Field strength in 500 MHz NMR ($0.5M) = 11.7 T

Field strength in 1 GHz NMR ($20M) = 23.5 T

Strongest continuous magnetic field = 45 T

(National High Magnetic Field Lab at Tallahassee, FL)

Slide6

Electrons in

p

, d, f orbitals

First-order perturbation theory

Bohr

magneton

9.724×10

−24

J/T

(2

l

+ 1)-fold

degeneracy

(field off)

Zeeman effect (field on)

Slide7

Quantum electrodynamics

g

-value

2.002319…

2-fold

degeneracy

(field off)

Electron spin

α

β

ESR or EPR (field on)

Slide8

Nuclear

g

-factor

p

roton: 5.586

2-fold

degeneracy

(field off)

Nuclear spin

α

β

NMR (field on)

Nuclear

magneton

1800 times smaller

than Bohr

magneton

P

roton

mass

Negative sign

positive nuclear charge

Slide9

Proton NMR

α

β

Sample

Sweep coils

Radio

freq

Slide10

Proton NMR spectra

Overall intensity

Groups of peaks

Relative intensities of groups of peaks

Pattern in each group (hyperfine structure)

Slide11

Overall intensity

α

β

Intensity of a NMR signal

~ energy of RF radiation absorbed / time

~ Δ

E ×

number of excess

α

spins

~

B

2

/

T

Stronger magnet + lower temperature

excess

α

spins

Slide12

Group of peaks: chemical shifts

Resonance freq.

Chemical shift

Resonance freq. of TMS

Si(CH

3

)

4

“ppm”

α

β

Slide13

Group of peaks: chemical shifts

Resonance freq.

Chemical shift

Shielding

constant

Slide14

Group of peaks: chemical shifts

Shielding

constant

+

Slide15

Group of peaks: chemical shifts

Shielding

constant

Slide16

Group of peaks: chemical shifts

14 12 10 8 6 4 2 0

δ

-COO

H

-C

H

O

Ar

-

H

ArO

H

RO

H

-C

H

-

-C

H

2

-

RC

H

3

Slide17

Relative intensities

C

2H6

O

H

H

2

H

3

OH

CH2

CH3

CH

3

CH

2

OH

RO

H

-C

H

2

-

RC

H

3

4 2 0

δ

Slide18

Hyperfine structure

CH

3

CH

2

OH

OH

CH

2

CH3

α

β

α

α

β

β

H

nearby H

Spin-spin coupling:

Slide19

Hyperfine structure

CH

3

CH

2

OH

OH

CH

2

CH

3

α

β

α

α

β

β

H

H

Spin-spin coupling:

ββ

α

α

βα, α

β

H

2

α

β

,

β

α

β

β

α

α

Slide20

Hyperfine structure

CH

3CH2

OH

OH

CH

2

CH

3

1

1

1

1

2

1

1

3

3

1

1

4

6

4

1

Pascal’s triangle

nearby H

nearby H

2

nearby H

3

nearby H

4

Slide21

CH

3

CH2OH

OH

CH

2

CH

3

Q

: Why doesn’t the proton in the OH group cause splitting?

A

: The proton undergoes a rapid exchange with protons in other ethanol or water molecules; its spin is indeterminate in the time scale of spectroscopic transitions; this causes lifetime broadening of spectral line rather than splitting.

?

Hyperfine structure

Slide22

CH

3

CH2OH

OH

CH

2

CH

3

Q

: Why is there no spin-spin coupling between the two protons in the CH

2

group?

A

: There

is

spin-spin coupling between them; however, its effect on the peaks is null and undetectable; this is because these protons are chemically and magnetically equivalent.

?

?

Hyperfine structure

Slide23

Hyperfine structure

CH

3CH2OH

Triplet

magnetic

Singlet

non-magnetic

no spin-spin coupling

with spin-spin coupling

No change in spacing

Slide24

Spin-spin coupling constant

H

H

H

C

H

H

C

C

H

Slide25

Spin-spin coupling constant

H

H

Fermi

contact

Fermi

contact

Covalent bond

singlet-coupling

higher energy??

Fermi contact

lower energy!

higher energy??

Slide26

Spin-spin coupling constant

H

C

Fermi

contact

Fermi

contact

Covalent

bond

singlet

coupling

H

Covalent

bond

singlet

coupling

Hund

Slide27

Spin-spin coupling constant

H

C

C

H

H

C

H

Martin

Karplus

Department of Chemistry

University of Illinois

ILLIAC

Karplus

equation

Image (c) University of Illinois

Slide28

Magnetic resonance imaging: MRI

Paul

Lauterbur

(far right)

Department of Chemistry

University of Illinois

Magnetic field gradient

Intensity

~ number of protons (in water) at

x

x

Resonance frequency

~ location (

x

)

Public domain image from Wikipedia

Slide29

Summary

We have studied the foundation of magnetic interactions and magnetic spectroscopy.

We have learned the theory of proton NMR as an essential tool for chemical structural analysis.The origins of chemical shifts, hyperfine structures, and spin-spin coupling constants are discussed as well as their relation to molecular structures.