🥼Organic Chemistry Unit 13 – NMR Spectroscopy for Structure Determination
NMR spectroscopy is a powerful tool for determining molecular structures. It uses the magnetic properties of certain atomic nuclei to provide detailed information about the chemical environment of individual atoms within a molecule.
This non-destructive technique analyzes pure compounds and mixtures without altering the sample. It requires NMR-active nuclei like 1H, 13C, 19F, and 31P, which possess spin and interact with external magnetic fields, producing spectra with signals corresponding to different chemical environments.
NMR spectroscopy utilizes the magnetic properties of certain atomic nuclei to determine the structure of molecules
Relies on the principle of nuclear magnetic resonance, where nuclei absorb and re-emit electromagnetic radiation in a magnetic field
Provides detailed information about the chemical environment of individual atoms within a molecule
Non-destructive technique that allows for the analysis of pure compounds and mixtures without altering the sample
Requires the presence of NMR-active nuclei, such as 1H, 13C, 19F, and 31P, in the molecule being analyzed
These nuclei possess a property called spin, which enables them to interact with external magnetic fields
Magnetic field strength is measured in units of Tesla (T) or MHz, with higher field strengths providing better resolution and sensitivity
Resulting NMR spectra display signals corresponding to different chemical environments of the NMR-active nuclei within the molecule
NMR-Active Nuclei and Their Properties
NMR-active nuclei have a non-zero spin quantum number (I), which determines their magnetic properties
Nuclei with even mass numbers and even atomic numbers (e.g., 12C, 16O) have I = 0 and are NMR-inactive
Nuclei with odd mass numbers (e.g., 1H, 13C, 19F) have I = 1/2 and are the most commonly used in NMR spectroscopy
The spin quantum number determines the number of possible orientations (2I + 1) of the nucleus in an external magnetic field
For I = 1/2 nuclei, there are two possible orientations: α (aligned with the field) and β (opposed to the field)
The energy difference between the α and β states is proportional to the strength of the external magnetic field (B0) and the gyromagnetic ratio (γ) of the nucleus
ΔE=2πhγB0, where h is Planck's constant
The gyromagnetic ratio is a constant for each NMR-active nucleus and determines its sensitivity and resonance frequency
The natural abundance of NMR-active isotopes varies, with 1H being the most abundant (99.98%) and 13C being relatively rare (1.11%)
This affects the sensitivity and acquisition time required for different nuclei
Chemical Shifts and Shielding Effects
Chemical shift (δ) is a measure of the resonance frequency of a nucleus relative to a standard reference compound
Expressed in parts per million (ppm) and is independent of the magnetic field strength
δ=νreferenceνsample−νreference×106, where ν is the resonance frequency
The chemical shift of a nucleus is determined by its chemical environment, which is influenced by the electron density surrounding the nucleus
Shielding effects occur when electrons circulate around the nucleus, generating a local magnetic field that opposes the external magnetic field
Increased electron density results in greater shielding and a lower (upfield) chemical shift
Decreased electron density leads to deshielding and a higher (downfield) chemical shift
Factors that influence shielding include electronegativity of neighboring atoms, hybridization, and the presence of aromatic rings
Electronegative atoms (e.g., O, N, F) withdraw electron density and cause deshielding
sp3 hybridized carbons are more shielded than sp2 and sp hybridized carbons
Aromatic rings generate a ring current that shields nearby nuclei
The chemical shift range for 1H NMR is typically 0-12 ppm, while 13C NMR has a wider range of 0-200 ppm
Spin-Spin Coupling and Multiplicity
Spin-spin coupling occurs when the magnetic moments of neighboring NMR-active nuclei interact with each other
Coupling between nuclei leads to the splitting of NMR signals into multiplets, with the number of peaks determined by the n+1 rule
n is the number of equivalent neighboring nuclei coupling to the observed nucleus
Multiplicity follows the pattern: singlet (n=0), doublet (n=1), triplet (n=2), quartet (n=3), etc.
Coupling constants (J) measure the strength of the interaction between coupled nuclei and are expressed in Hertz (Hz)
J is independent of the magnetic field strength and can provide information about bond angles and stereochemistry
First-order coupling occurs when the chemical shift difference between coupled nuclei is much larger than the coupling constant
Results in symmetrical multiplets with predictable peak intensities based on Pascal's triangle
Second-order coupling arises when the chemical shift difference is comparable to the coupling constant
Leads to more complex, asymmetric multiplets and roofing effects
Homonuclear coupling involves the interaction between the same type of nuclei (e.g., 1H-1H), while heteronuclear coupling occurs between different types of nuclei (e.g., 1H-13C)
Coupling can be transmitted through bonds (scalar coupling) or through space (dipolar coupling)
Scalar coupling is more common and is used to determine the connectivity of atoms in a molecule
1D Proton NMR Spectra Interpretation
1D 1H NMR is the most common type of NMR experiment and provides a wealth of structural information
The number of signals in a 1H NMR spectrum indicates the number of distinct chemical environments for hydrogen atoms in the molecule
Signal integration measures the relative number of hydrogen atoms contributing to each peak
The area under each signal is proportional to the number of hydrogen atoms in that environment
Integration values are typically normalized to the smallest integer value
Multiplicity of signals arises from spin-spin coupling and provides information about the number of neighboring hydrogen atoms
Coupling constants can be measured as the distance between peaks in a multiplet and provide information about bond angles and stereochemistry
The chemical shift of signals is influenced by the electron density around the hydrogen atoms and can be used to identify functional groups
For example, aldehydic protons appear around 9-10 ppm, aromatic protons around 6-8 ppm, and aliphatic protons around 0-4 ppm
Exchangeable protons (e.g., -OH, -NH) may appear as broad signals or be absent due to rapid exchange with solvent molecules
Interpretation of 1H NMR spectra involves correlating the observed signals with the structure of the molecule, considering the number of signals, integration, multiplicity, and chemical shifts
13C NMR Spectroscopy
13C NMR spectroscopy provides complementary information to 1H NMR and is particularly useful for determining the carbon skeleton of a molecule
The low natural abundance of 13C (1.11%) results in lower sensitivity compared to 1H NMR
Requires longer acquisition times or higher sample concentrations to obtain good signal-to-noise ratios
13C NMR spectra typically display single peaks for each unique carbon environment, as the probability of two 13C nuclei being adjacent to each other is very low
The chemical shift range for 13C NMR is much wider than for 1H NMR, spanning from 0-200 ppm
Allows for better resolution and differentiation of carbon environments
Factors influencing 13C chemical shifts include hybridization, electronegativity of neighboring atoms, and the presence of multiple bonds
sp3 hybridized carbons appear around 0-80 ppm, sp2 carbons around 100-150 ppm, and sp carbons around 60-90 ppm
Electronegative substituents cause a downfield shift in the 13C signal
Double and triple bonds also result in downfield shifts
Broadband decoupling is often employed in 13C NMR to simplify the spectra by removing the effects of 1H-13C coupling
Results in singlets for each carbon environment, facilitating interpretation
13C NMR can be used to identify quaternary carbons, which are not directly observable in 1H NMR due to the absence of attached hydrogen atoms
Comparison of 13C NMR chemical shifts with reference data and prediction tools can aid in structural elucidation
Advanced NMR Techniques
2D NMR experiments provide additional information about the connectivity and spatial relationships between nuclei in a molecule
Common 2D techniques include COSY, HSQC, HMBC, and NOESY
COSY (COrrelation SpectroscopY) identifies scalar coupling between protons, helping to establish the connectivity of the carbon skeleton
Cross-peaks in a COSY spectrum indicate protons that are coupled to each other
HSQC (Heteronuclear Single Quantum Coherence) correlates protons with directly attached carbons
Useful for assigning carbon signals and identifying the number of hydrogen atoms attached to each carbon
HMBC (Heteronuclear Multiple Bond Correlation) detects long-range coupling between protons and carbons, typically 2-4 bonds apart
Helps to establish the connectivity of the molecule and identify quaternary carbons
NOESY (Nuclear Overhauser Effect SpectroscopY) identifies protons that are spatially close to each other, even if not directly bonded
Useful for determining the relative stereochemistry and conformation of molecules
DEPT (Distortionless Enhancement by Polarization Transfer) experiments selectively enhance the signals of CH, CH2, and CH3 groups in 13C NMR
Helps to identify the number of hydrogen atoms attached to each carbon
Quantitative NMR (qNMR) techniques allow for the accurate determination of sample concentration and purity
Requires the use of an internal standard with a known concentration and a long relaxation delay to ensure complete relaxation of all nuclei
Solid-state NMR spectroscopy enables the analysis of samples that are not soluble or are in the solid phase
Techniques such as magic angle spinning (MAS) and cross-polarization (CP) are employed to improve resolution and sensitivity
Solving Unknown Structures with NMR Data
Determining the structure of an unknown compound using NMR data involves a systematic approach that combines information from various NMR experiments
Begin by analyzing the 1D 1H NMR spectrum to identify the number of distinct hydrogen environments, their chemical shifts, multiplicities, and coupling constants
Use the integration values to determine the relative number of hydrogen atoms in each environment
Compare the observed chemical shifts with reference data to identify potential functional groups and structural features
Analyze the 13C NMR spectrum to determine the number of unique carbon environments and their chemical shifts
Use DEPT experiments to identify the number of hydrogen atoms attached to each carbon
Combine the information from 1H and 13C NMR to construct fragments of the molecule and establish connectivity
Use 2D NMR experiments to confirm the connectivity and spatial relationships between atoms
COSY and TOCSY help establish the proton-proton connectivity
HSQC correlates protons with directly attached carbons
HMBC identifies long-range proton-carbon correlations, helping to connect fragments and identify quaternary carbons
NOESY experiments can provide information about the relative stereochemistry and conformation of the molecule
Consider the molecular formula, which can be obtained from mass spectrometry or elemental analysis, to ensure that the proposed structure is consistent with the data
Use NMR prediction software to compare the observed chemical shifts and coupling constants with those predicted for the proposed structure
Iterate the process, refining the structure based on any inconsistencies or additional information until a final structure is determined that satisfies all the available data
Confirm the structure through comparison with literature data, if available, or by synthesizing the compound and comparing its NMR spectra with the unknown sample