1d nmr spectroscopy

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1D NMR Spectroscopy Chemistry 355 Fall 2010 Note: Most figures are from Silverstein, Webster and Kiemle, 7/e, while others are from the Web. While sources are not cited for space limitations, the author claims no credit or copyright for any of these unless specifically noted.

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  • 1D NMR Spectroscopy

    Chemistry 355

    Fall 2010

    Note: Most figures are from Silverstein, Webster and Kiemle, 7/e, while others

    are from the Web. While sources are not cited for space limitations, the author

    claims no credit or copyright for any of these unless specifically noted.

  • Principles of Magnetic Resonance

    Nuclear spin (angular momentum)

    Based on nuclear particles (each has spin )

    Must have odd number of protons, neutrons, or both

    I = 0; 12C not NMR active

    I = ; 1H, 13C, 15N, 31P, 19F, 29Si

    I = 1; 2H, 14N

    I = 5/2; 17O

  • Principles of Magnetic Resonance

    Spins orient in a magnetic field

    Small proportion

    DE = (hg/2p)B0

    Radio frequency low energy transition

    At 298K and 2.35 T (100 MHz) only 0.00041% of protons in a given sample

    are excitable.

    Difference is greatest at low temperature

  • Principles of Magnetic Resonance

    Spins precess about the magnetic field at a

    characteristic frequency

    Larmor frequency

    n1 = (g/2p)B0

  • Principles of Magnetic Resonance

    (a,b) - By irradiating with Rf energy, we can flip the magnetic moment of a nucleus or nuclei (move it from

    vertical)

    (c, d) - As the nucleus recovers, it will emit its Larmor frequency as a

    damped oscillation called a free

    induction decay (FID)

    (d)

    Rf

    pulse

    FID

    Immediately

    After

    pulse

    Before

    pulse

  • Magnets Field 1 T = 10,000 gauss Earth 0.3 gauss Permanent magnets

    0.1 T (5 MHz) to 2.35 T (100 MHz) Limited by bulk and materials

    Electromagnet Normal Superconducting

    4.7 T (200 MHz) to 22.3 T (950 MHz)

    Cryocooled

    Frequency Proportional to field Different for nuclei Spectrometer frequency usually

    expressed for 1H

    60 MHz at 1.4 T 400 MHz at 9.4 T 950 MHz at 22.3 T 13C frequency that of 1H

  • The NMR Spectrometer

    Magnet Mini radio station

    Transmitter Receiver Amplifier Digitizer (FT) Computer (FT)

    transmitter receiver

    Sweep

    Generator

    amplifier

    preamplifier

    The Magnet and

    Spectrometer work

    together, but are

    independent.

    Any magnet can be used with either pulsed FT or continuous wave NMR

  • The Basic 1D NMR Experiment Continuous wave

    Sweep frequency

    Nuclei ring at their resonant frequency

    First spectrum 1951

  • The Basic 1D NMR Experiment Fourier transform

    All frequencies pulsed simultaneously

    (Heisenberg)

    Listen to all sing back at once - Free Induction

    Decay (FID)

    Fourier transform

    Time to Frequency

    Greater sensitivity

    Time averaging

  • The Basic 1D NMR Experiment

  • The Effect of Field

    Coupling frequency is a constant (Hz)

    Higher frequency = more Hz/ppm

    Higher field gives

    Higher resolution

    Greater sensitivity

    0123PPM

    0123PPM

    0123PPM

    0123PPM

    0123PPM

    60 MHz

    100 MHz

    200 MHz

    400 MHz

    800 MHz

  • -1012345PPM

    The Effect of Field

    012345PPM

    012345PPM

    60 MHz

    400 MHz

    800 MHz

    HO

  • Chemical Shift - d Position on frequency scale

    Expressed in ppm to make it field independent

    Influenced by Electron density about atom

    Electronegative atoms deshield

    Silicon shields

    Organometallics

    Anisotropic effects Double bonds deshield

    Triple bonds shield

    Correlation charts

    Best discussion in Carey

  • Integration Area under peak is

    proportional to relativenumbers of atoms

    Accuracy to ~1-5%

    Depends strongly on acquisition parameters Relaxation time

    Proton integrates

    Carbon does not (usually)

  • 1H-1H Through-bond (J) Coupling Coupled via electron spins

    Distance between peaks in Hz First two peaks is always 1st J

    Up to five bonds away

    2-bond (geminal)

    3-bond (vicinal)

    4-bond (allylic)

    Same both ways (J1,2 = J2,1)

    OH, NH solvent dependent, exchangeable

    Pascals triangle n + 1 rule

    Only holds if all J identical

    Pentet (p)

    (sxt)

    (spt)

    (o)

    (n)

    0123PPM

    7 Hz

    7 Hz

    CH3CH2OH

  • 1H-1H Through-bond (J) Coupling Magnitudes vary 0-20 Hz

    2J>=3J>4J>5J

    Free rotation ~7-10 Hz

    For hindered rotation J depends on dihedral angle

    Karplus relationship Largest at 0o, 180o

    Smallest around 80o-90o

    Different relationship for 2, 3, and 4 bond

    NH2

    H

    NH2

    H

    NH2

    NH2

    NH2

    NH2

    NH2

    NH2

    H

    NH2

    H

    NH2

    180o

    Large J30o

    Small J

  • 1H-1H Through-bond (J) Coupling Nonstandard couplings doublet of doublets (dd)

    11 Hz

    18 Hz

  • 1H-1H Through-bond (J) Coupling

    Nonstandard couplings doublet of quartets (dq)

    5 Hz

    8 Hz

  • 1H-1H Through-bond (J) Coupling

    Nonstandard couplings (dqd)

  • 1H-1H Through-bond (J) Coupling

    Look for basic patterns to get couplings

  • 1H-X Through-bond (J) Coupling Other magnetically active nuclei

    13C, 15N, 31P, 19F, 29Si

    Metals 6Li, 51V, 195Pt, 199Hg

  • 13C NMR Same arguments apply as with 1H

    Pulse, observe FT for spectrum Larger Sweep width Less sensitivity

    1.11% 13C

    Chemical shift Electronegative atoms Anisotropic effects

    No integration Except quant 13C Long pulse delay

    Coupling with protons Decoupling

  • 13C NMR Decoupling

    Irradiate 1H while acquiring 13C

    Can be continuous or pulsed

    Inverse gated decoupling

  • DEPT Editiing Distortionless Enhancement through

    Polarization Transfer Irradiate 1H while acquiring 13C

    Can be continuous or pulsed

    Pulse widths

    45o CH, CH2, CH390o CH only

    135o CH2 up, CH3, CH down

    Normal

    Decoupled13C

    DEPT 90

    DEPT 135

  • DEPT Editing Distortionless Enhancement through

    Polarization Transfer Irradiate 1H while acquiring 13C

    Can be continuous or pulsed

    Pulse angle q

    45o CH, CH2, CH390o CH only

    135o CH2 up, CH3, CH down

    Normal

    Decoupled13C

    DEPT 90

    DEPT 135

  • Summary of Information from NMR

    NMR 1H

    Chemical Shift what kind of protons

    Integration how many protons and in what groups

    Couplings

    how many neighbors (n+1)

    Which neighbors (J values)

    13C How many carbons (normal decoupled)

    How many protons (coupled or DEPT)

    2D spectra direct connectivity (9/21)

  • General Notes on Structure Elucidation of

    Synthetic Materials from Spectroscopy Some techniques yield lots of information. Others may not yield as much but may give critical information.

    NMR protons, carbons. connectivity IR functional groups MS mol. wt., structural fragments UV-Vis absorbing moieties, esp. aromatics (Characteristic lmax)

    Use all the information you can get Reaction info

    Compare to starting material to see what has changed Compare to expected data for expected product based on structure Look at possible alternate products based on the reactants/reagents used Be on the lookout for impurities

    Starting material and co-reactants Solvents Workup reagents/solvents Cleaning solvents and grease

    These are all interactive. You may need to go back and forth a few times to settle on a logical structure

    Any structure you propose should agree with all characterization data.

  • Spectroscopy Homework

    (Silverstein) 1.1-1.3

    2.2

    3.1, 4.1 No Pople notation

    Label equivalent proton groups

    Label equivalent carbons

    3.10 a Determine splitting pattern and coupling constants

    3.4, 4.4 a-d Give structure and assign resonances for proton, carbon, IR and mass spectra to the best of your ability

    Due 9/13