Sensitivity in NMR is quantified by the signal-to-noise ratio (S/N).
Several factors influence S/N:
N: Number of spins (concentration)
γ: Gyromagnetic ratio of detected nuclei
n: Number of scans
B: External magnetic field
Formula: S/N∝Nγ3B3n
An example comparing a 750 MHz spectrometer with a 300 MHz spectrometer, illustrating the improvement in sensitivity with a higher magnetic field:
(300750)23=cN</em>2N<em>1
NMR Sensitivity: Magnetic Field Strength
Increasing magnet strength (B0) is a major way to increase sensitivity.
Approximate costs:
~$2,00,000
~$4,500,000
Formula: S/N∝Nγ3B3n
NMR Sensitivity: Concentration
Increasing the concentration of the sample is a common approach to increase sensitivity.
Example comparing two different concentrations on signal to noise ratio.
Formula: S/N∝Nγ3B3n
NMR Sensitivity: Gyromagnetic Ratio and Natural Abundance
The gyromagnetic ratio (γ) and the natural abundance of the isotope significantly affect NMR sensitivity.
(γH/γC)3 for 13C is 64x
(γH/γN)3 for 15N is 1000x
1H is approximately 64 times as sensitive as 13C and 1000 times as sensitive as 15N.
Considering the natural abundance:
13C has a natural abundance of 1.1%.
15N has a natural abundance of 0.37%.
Relative sensitivity increases to ~6,400x and ~2.7x105x, respectively.
1H NMR spectra of caffeine (8 scans ~12 secs)
13C NMR spectra of caffeine (8 scans ~12 secs)
13C NMR spectra of caffeine (10,000 scans ~4.2 hours)
Formula: S/N∝Nγ3B3n
NMR Sensitivity: Number of Scans
Increasing the number of scans (NS) or signal averaging is a common approach to increase sensitivity and signal-to-noise ratio (S/N).
S/N≈n
S/N∝Nγ3B3n
The S/N increases with the square root of the number of scans.
Comparison of number of Scans and S/N:
n = 1, S/N = 1
n = 8, S/N = 2.83
n = 16, S/N = 4
n = 80, S/N = 8.94
n = 800, S/N = 28.3
Experimental Time = Number of Scans x Acquisition Time, so it takes significantly longer to acquire the spectrum as the number of scans increase.
Solvent Selection in NMR
The ideal solvent should:
Contain no protons
Be inert
Have a low boiling point
Be inexpensive
Deuterated solvents are necessary for modern NMR instruments:
Deuterium signal is used to lock or stabilize the B0 field of the magnet.
Instruments with a deuterium channel constantly monitor and adjust (locks) the B0 field to the frequency of the deuterated solvent.
The deuterium signal is also used to shim the B0 field, ensuring the homogeneity of the field is precise at the center of the sample.
Commonly used deuterated solvents: CDCl3, C6D6.
NMR Sample Preparation
Shows a picture of NMR Sample Preparation and a 500MHZ/52 MM setup.
NMR Spectra Analysis
This section details the analysis of an NMR spectrum.
Spectrum for ethylacetate.
Key parameters:
Experiment = zg.ppg
Pulse length = 22.00 usec
Recycle delay = 3.00 sec
Number of acquisitions (NA) = 8
Points (PTS1d) = 8192
F1 = 90.019463 MHZ
SW1 = 1470.60 Hz
AT1 = 5.57 sec
Hz per Pt 1stD = 0.18 Hz
01 = 495.40
LB1 = 0.00 Hz
TP A = -75.50
B
-76.30
Peaks at:
4.159 ppm
4.079 ppm
2.032 ppm
Spectrum includes signals for H3C and CH3 groups.
NMR: Spectrum Concepts
Key concepts in NMR spectrum analysis:
Shielding and deshielding
Chemical Shift (ppm)
Number of Signals
Integral of Signals
Coupling Constant (Hz)
Understanding Magnetic Anisotropy
Chemical Shift
Explains why hydrogen atoms have different frequencies.
ν=2πγB0
B0 is 300, 400, or 600 MHz.
Chemical Shift: Shielding
Nuclei are surrounded by electrons, which generate a magnetic field that alters the B0 field in the microenvironment around the nucleus; this is called SHIELDING of the nucleus.
Shielding (σ) varies with chemical environments.
Electrons move to create an opposing field.
1 T = 10 kG
For Naked Nuclei: ν=2πγB0
Effective magnetic field: B<em>eff=B</em>0−σ
Chemical Shift: Shielding (Continued)
At a constant applied magnetic field (B0), different protons experience different effective magnetic fields (Beff).
Electronic shielding σ is normally positive.
The shielding constant (σ) is closely related to the degree of electron density surrounding the nucleus.
Nuclei in regions of high electron density are shielded.
Conversely, nuclei in low electron density are deshielded.
Variation of the resonance frequency with shielding has been termed the Chemical Shift.
Example calculation:
νeff=299.999994MHz
ν=2πγBeff=300MHz
Δν=6.0Hz
Δν=2πγσB0
Chemical Shift: ppm (parts per million)
The basic frequency of the pulse (B1) is not the same as the sample resonance.
The observed FID (Free Induction Decay) is the difference of two frequencies: the B1 (radiofrequency, known) and the frequency emitted by excited nuclei.
These differences in resonance frequency are very small (Hz) compared with B1 (MHz).
The unit of chemical shift is ppm (parts per million).
No attempt is made to measure the exact resonance frequency of any proton.
Different machines have different real chemical shifts (ppm).
A standard reference is used: tetramethylsilane (TMS, Me4Si).
The chemical shift δ expresses the amount by which a proton resonance is shifted from TMS, in parts per million, of the spectrometer’s basic operating frequency.
It is a field-independent measure.
Variation of the resonance frequency with shielding has been termed the Chemical Shift.
The chemical shift in ppm is independent of the strength of the applied magnetic field.
Formula: ν=δ∗xHz
Example: for a 400 MHz machine with δ = 2.0 ppm, ν=2.0∗400Hz=800Hz
Formulas:
δ=x</em>MHzν<em>Hz
ν=δ<em>ppm∗x</em>MHz=δ∗10−6∗x∗106Hz=δ∗xHz
δ=xMHzν<em>sample−ν</em>TMS
Chemical Shift unit: ppm vs Hz
ν=δ∗xHz
The same chemical shift (e.g., 2.032 ppm) in ppm will have a different frequency under different magnetic fields.
Stronger magnetic field, higher chemical shift in Hertz.
Examples:
B0 = 90 MHz: ν=2.032∗90Hz=182.88Hz
B0 = 400 MHz: ν=2.032∗400Hz=812.8Hz
Effect of Changing Field Strength
The strongest Magnetic field available should be used to spread out the chemical shifts.
ν=δ∗xHz
Range of Chemical Shifts (δ)
Different nuclei have different shift ranges, depending on γ.
Nucleus Shift Range (ppm) Reference
1H -30 to 20 (commonly 0-12) (CH3)4Si
13C -100 to 200 (commonly 0-220) (CH3)4Si
19F -200 to 200 CFCl3
31P -100 to 250 H3PO4
Δν=2πγσB0
Downfield and Upfield
Downfield: Deshielded nuclei. Higher frequency. Larger effective magnetic field.
Upfield: Shielded nuclei. Lower frequency. Smaller effective magnetic field.
Protons in a molecule
More shielded protons absorb at a higher field (upfield).
Less shielded protons absorb at a lower field (downfield).
Examples include H-C-O and H-O-C-H.
Proton NMR Chemical Shifts of Common Functional Groups & Factors
Electronegativity
Anisotropy (Ring Currents)
Electron Delocalization
H‐Bonding
Proton NMR Chemical Shifts of Common Functional Groups
Ranges of chemical shifts for different types of protons:
OH : 12 - 1
Y-C-H: F, etc 4 - 2
C=O -C-H: 10 - 9
C-H: 5 - 0
Regions:
Deshielded, High Frequency, High Chemical Shift, Downfield
Shielded, low Frequency, Low Chemical Shift, Upfield
H-Bonding
anisotropy
Electronegativity
Factors on Chemical Shift: Electron density
Electronegativity
Anisotropy (π-bond)
Electron Delocalization
H-Bonding
Deshielding by Electronegative Element
Chlorine “deshields” the proton by taking valence electron density away from carbon, which in turn takes more density from hydrogen.
“highly shielded” protons appear at upfield (lower δ).
“deshielded“ protons appear at downfield (higher δ).
deshielding moves proton resonance to lower field and higher δ.
Cδ+−Hδ−Clδ−
Deshielding by Electronegative Element examples
The effect increases with greater numbers of electronegative atoms:
CHCl3: 7.27 ppm
CH2Cl2: 5.30 ppm
CH3Cl: 3.05 ppm
The effect decreases with increasing distance from the electronegative atom:
−CH2−Br: 3.30 ppm
−CH2−CH2−Br: 1.69 ppm
− CH2−CH2−CH2−Br: 1.25 ppm
The effect completely vanishes at the fourth bond from the electronegative atom.
Proton NMR Chemical Shifts of Common Functional Groups (slide 2)
Common Functional Groups Examples
Unexpected Shielding
H-C-OR
| C=C
H 5.5 ppm
H-C=CR.
2.0 ppm
Diamagnetic Anisotropic effect DUE TO THE PRESENCE OF -BONDS
The presence of a nearby pi bond or pi system greatly affects the chemical shift.
Induced magnetic fields due to the - electrons have greatest effect.
Diamagnetic Anisotropy
Shielding and deshielding depend on the orientation of the molecule with respect to the applied magnetic field.
Electron density of chemical bonds could be higher in one direction than another: anisotropic
Nuclei in close proximity of these bonds could be affected
Most pronounced in delocalised π‐ systems
For example H-C≡C-H Shielding of alkyne protons Shielded δ = 2.5 ppm shielded
Diamagnetic Anisotropy: Aldehyde δ = 9-10 ppm
Shielding and deshielding depend on the orientation of the molecule with respect to the applied magnetic field.
Deshielding of aldehyde protons
The effect of B0 is greatest along the transverse axis of the C=O.
Diamagnetic Anisotropy: Aldehyde spectrum
Displays a spectrum of benzaldehyde, showing a peak at 9.984 ppm for the aldehyde proton.
Diamagnetic Anisotropy: Alkene δ = 5-6 ppm
The induced field reinforces the external field (deshielding).
Shows the anisotropic effect in alkenes.
Diamagnetic Anisotropy: Alkene examples
Examples:
H/δ = 5-6 ppm
8 = 2.2 ppm
C
8 = 2.2 ppm H
Diamagnetic Anisotropy: Alkene values
Shows chemical shift values of miscellaneous Alkenes
Diamagnetic Anisotropy: Ketone δ = 2-2.5 ppm
Examples for methyl, methylene groups.
Diamagnetic Anisotropy: Ketone explanation
The magnetic anisotropy of C=O has a strongly deshielding (+δ) region in the plane of the carbonyl group.
Diamagnetic Anisotropy: π-bond shielding
Chemical shifts values and deshielding.
Proton NMR Chemical Shifts of Common Functional Groups (slide 3)
Chemical shifts values and deshielding.
Diamagnetic Anisotropy: Aromatic
Protons on the benzene ring are deshielded.
Benzene ring contains delocalized -electrons
Deshielded δ = 7-8 ppm.
Diamagnetic Anisotropy: Aromatic example
Displays a spectrum of styrene, showing signals in the aromatic region (7-8 ppm) and alkene region (5-6 ppm).
Examples of Ring-Current Effect
Shows multiple examples of ring-current effects on chemical shifts in various aromatic compounds, with specific chemical shift values listed for different protons.
Reinforced double Diamagnetic Anisotropy
All the ring protons of acetophenone are deshielded because of the ring current effect.