lecture 37 nuclear magnetic resonance

29
Lecture 37 Nuclear magnetic resonance

Upload: zanna

Post on 24-Feb-2016

28 views

Category:

Documents


0 download

DESCRIPTION

Lecture 37 Nuclear magnetic resonance. Nuclear magnetic resonance. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Lecture 37 Nuclear magnetic resonance

Lecture 37Nuclear magnetic resonance

Page 2: Lecture 37 Nuclear magnetic resonance

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.

Page 3: Lecture 37 Nuclear magnetic resonance

Circular electric current = magnet

Electrons in p, d, f orbitalsElectron spinNuclear spin

angular momentum

charge

magneticmoment

mass

Page 4: Lecture 37 Nuclear magnetic resonance

Magnet-magnetic-field interactionhigh energy

low energy

Classical

Magnetic moment

Magnetic field

Quantum

Page 5: Lecture 37 Nuclear magnetic resonance

Tesla

Nikola TeslaPublic domain image from Wikipedia

kgm2/s

C

J

kg

T (Tesla)

1 T = 1 V s / m2

Field strength in 500 MHz NMR ($0.5M) = 11.7 TField strength in 1 GHz NMR ($20M) = 23.5 T

Strongest continuous magnetic field = 45 T(National High Magnetic Field Lab at Tallahassee, FL)

Page 6: Lecture 37 Nuclear magnetic resonance

Electrons in p, d, f orbitalsFirst-order perturbation theory

Bohr magneton 9.724×10−24 J/T

(2 l + 1)-fold degeneracy

(field off)

Zeeman effect (field on)

Page 7: Lecture 37 Nuclear magnetic resonance

Quantum electrodynamics

g-value2.002319…

2-fold degeneracy

(field off)

Electron spin

α

βESR or EPR (field on)

Page 8: Lecture 37 Nuclear magnetic resonance

Nuclear g-factorproton: 5.586

2-fold degeneracy

(field off)

Nuclear spin

α

β

NMR (field on)

Nuclear magneton 1800 times smaller

than Bohr magnetonProtonmass

Negative signpositive nuclear charge

Page 9: Lecture 37 Nuclear magnetic resonance

Proton NMR

α

β

Sample

Sweep coils

Radio freq

Page 10: Lecture 37 Nuclear magnetic resonance

Proton NMR spectra(1) Overall intensity(2) Groups of peaks(3) Relative intensities of groups of peaks(4) Pattern in each group (hyperfine structure)

Page 11: Lecture 37 Nuclear magnetic resonance

Overall intensity

α

β

Intensity of a NMR signal ~ energy of RF radiation absorbed / time~ ΔE × number of excess α spins~ B2 / T

Stronger magnet + lower temperature

excess α spins

Page 12: Lecture 37 Nuclear magnetic resonance

Group of peaks: chemical shiftsResonance freq.

Chemical shift

Resonance freq. of TMSSi(CH3)4

“ppm”

α

β

Page 13: Lecture 37 Nuclear magnetic resonance

Group of peaks: chemical shiftsResonance freq.

Chemical shift

Shieldingconstant

Page 14: Lecture 37 Nuclear magnetic resonance

Group of peaks: chemical shifts

Shieldingconstant

+

Page 15: Lecture 37 Nuclear magnetic resonance

Group of peaks: chemical shiftsShieldingconstant

Page 16: Lecture 37 Nuclear magnetic resonance

Group of peaks: chemical shifts

14 12 10 8 6 4 2 0 δ

-COOH-CHO

Ar-HArOH

ROH-CH-

-CH2-

RCH3

Page 17: Lecture 37 Nuclear magnetic resonance

Relative intensitiesC2H6O

H H2 H3OH CH2

CH3

CH3CH2OH

ROH-CH2-

RCH3

4 2 0 δ

Page 18: Lecture 37 Nuclear magnetic resonance

Hyperfine structure

CH3CH2OH

OH CH2 CH3

α

βα

α

β

β

H nearby HSpin-spin coupling:

Page 19: Lecture 37 Nuclear magnetic resonance

Hyperfine structure

CH3CH2OH

OH CH2 CH3

α

βα

α

β

β

H HSpin-spin coupling:

ββ

ααβα, αβ

H2

αβ, βαββ

αα

Page 20: Lecture 37 Nuclear magnetic resonance

Hyperfine structure

CH3CH2OH

OH CH2 CH3

1

1 1

1 2 1

1 3 3 1

1 4 6 4 1

Pascal’s triangle

nearby H

nearby H2

nearby H3

nearby H4

Page 21: Lecture 37 Nuclear magnetic resonance

CH3CH2OH

OH CH2 CH3

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

Page 22: Lecture 37 Nuclear magnetic resonance

CH3CH2OH

OH CH2 CH3

Q: Why is there no spin-spin coupling between the two protons in the CH2 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

Page 23: Lecture 37 Nuclear magnetic resonance

Hyperfine structure

CH3CH2OHTripletmagnetic

Singletnon-magnetic

no spin-spin coupling with spin-spin coupling

No change in spacing

Page 24: Lecture 37 Nuclear magnetic resonance

Spin-spin coupling constant

H H

H C H

H C C H

Page 25: Lecture 37 Nuclear magnetic resonance

Spin-spin coupling constantH H

Fermicontact

Fermicontact

Covalent bondsinglet-coupling

higher energy??Fermi contactlower energy!

higher energy??

Page 26: Lecture 37 Nuclear magnetic resonance

Spin-spin coupling constant

H C

Fermicontact

Fermicontact

Covalentbond

singletcoupling

H

Covalentbond

singletcoupling

Hund

Page 27: Lecture 37 Nuclear magnetic resonance

Spin-spin coupling constant

H C C H

H

C H

Martin KarplusDepartment of Chemistry

University of Illinois ILLIAC

Karplus equation

Image (c) University of Illinois

Page 28: Lecture 37 Nuclear magnetic resonance

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

Page 29: Lecture 37 Nuclear magnetic resonance

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.