Nuclear Magnetic Resonance A Introduction Nuclear Magnetic Resonance

Nuclear Magnetic Resonance A. ) Introduction: Nuclear Magnetic Resonance (NMR) measures the absorption of electromagnetic radiation in the radio-frequency region (~4 -900 MHz) - nuclei (instead of outer electrons) are involved in absorption process - sample needs to be placed in magnetic field to cause different energy states NMR was first experimentally observed by Bloch and Purcell in 1946 (received Nobel Prize in 1952) and quickly became commercially available and widely used. Probe the Composition, Structure, Dynamics and Function of the Complete Range of Chemical Entities: from small organic molecules to large molecular weight polymers and proteins. NMR is routinely and widely used as the preferred technique to rapidly elucidate the chemical structure of most organic compounds. One of the MOST Routinely used Analytical Techniques

NMR History 1937 1946 1953 1966 1975 1985 Rabi predicts and observes nuclear magnetic resonance Bloch, Purcell first nuclear magnetic resonance of bulk sample Overhauser NOE (nuclear Overhauser effect) Ernst, Anderson Fourier transform NMR Jeener, Ernst 2 D NMR Wüthrich first solution structure of a small protein (BPTI) from NOE derived distance restraints 1987 3 D NMR + 13 C, 15 N isotope labeling of recombinant proteins (resolution) 1990 pulsed field gradients (artifact suppression) 1996/7 new long range structural parameters: - residual dipolar couplings from partial alignment in liquid crystalline media - projection angle restraints from cross-correlated relaxation TROSY (molecular weight > 100 k. Da) Nobel prizes 1944 Physics Rabi (Columbia) 1952 Physics Bloch (Stanford), Purcell (Harvard) 1991 Chemistry Ernst (ETH) 2002 Chemistry Wüthrich (ETH) 2003 Medicine Lauterbur (University of Illinois in Urbana ), Mansfield (University of Nottingham)

NMR History First NMR Spectra on Water 1 H NMR spectra of water Bloch, F. ; Hansen, W. W. ; Packard, M. The nuclear induction experiment. Physical Review (1946), 70 474 -85.

NMR History First Observation of the Chemical Shift 1 H NMR spectra ethanol Modern ethanol spectra Arnold, J. T. , S. S. Dharmatti, and M. E. Packard, J. Chem. Phys. , 1951. 19: p. 507.

Typical Applications of NMR: 1. ) Structural (chemical) elucidation > Natural product chemistry > Synthetic organic chemistry - analytical tool of choice of synthetic chemists - used in conjunction with MS and IR 2. ) Study of dynamic processes > reaction kinetics > study of equilibrium (chemical or structural) 3. ) Structural (three-dimensional) studies > Proteins, Protein-ligand complexes > DNA, RNA, Protein/DNA complexes > Polysaccharides 4. ) Drug Design > Structure Activity Relationships by NMR 5) Medicine -MRI images of the Human Brain Taxol (natural product) NMR Structure of MMP-13 complexed to a ligand

Each NMR Observable Nuclei Yields a Peak in the Spectra “fingerprint” of the structure 2 -phenyl-1, 3 -dioxep-5 -ene 1 H NMR spectra 13 C NMR spectra

Information in a NMR Spectra Observable Name Quantitative Information d(ppm) = uobs –uref/uref (Hz) chemical (electronic) environment of nucleus peak separation (intensity ratios) neighboring nuclei (torsion angles) Peak position Chemical shifts (d) Peak Splitting Coupling Constant (J) Hz Peak Intensity Integral unitless (ratio) relative height of integral curve nuclear count (ratio) T 1 dependent Peak Shape Line width Du = 1/p. T 2 peak half-height molecular motion chemical exchange uncertainty principal uncertainty in energy

A Basic Concept in Electro. Magnetic Theory A Direct Application to NMR A perpendicular external magnetic field will induce an electric current in a closed loop An electric current in a closed loop will create a perpendicular magnetic field

Theory of NMR Quantum Description Nuclear Spin (think electron spin) l a) Nucleus rotates about its axis (spin) a) Nuclei with spin have angular momentum (p) 1) quantized, spin quantum number I 2) 2 I + 1 states: I, I-1, I-2, …, -I 3) identical energies in absence of external magnetic field c) NMR “active” Nuclear Spin (I) = ½: 1 H, 13 C, 15 N, 19 F, 31 P Odd atomic mass I = +½ & -½ NMR “inactive” Nuclear Spin (I) = 0: 12 C, 16 O Even atomic mass & number Quadrupole Nuclei Nuclear Spin (I) > ½: 14 N, 2 H, 10 B Even atomic mass & odd number I = +1, 0 & -1

Magnetic Moment (m) a) spinning charged nucleus creates a magnetic field Magnetic moment Similar to magnetic field created by electric current flowing in a coil b) magnetic moment (m) is created along axis of the nuclear spin m = gp where: p – angular momentum g – gyromagnetic ratio (different value for each type of nucleus) c) magnetic moment is quantized (m) m = I, I-1, I-2, …, -I for common nuclei of interest: m = +½ & -½

Magnetic alignment = g h / 4 p Bo In the absence of external field, each nuclei is energetically degenerate Add a strong external field (Bo). and the nuclear magnetic moment: aligns with (low energy) against (high-energy)

Energy Levels in a Magnetic Field a) Zeeman Effect -Magnetic moments are oriented in one of two directions in magnetic field b) Difference in energy between the two states is given by: DE = g h Bo / 2 p where: Bo – external magnetic field units: Tesla (Kg s-2 A-1) h – Planck’s constant 6. 6260 x 10 -34 Js g – gyromagnetic ratio unique value per nucleus 1 H: 26. 7519 x 107 rad T-1 s 2 p (observed NMR frequency) c) Frequency of absorption: n = g Bo / d) From Boltzmann equation: Nj/No = exp(-gh. Bo/2 pk. T)

Energy Levels in a Magnetic Field • Transition from the low energy to high energy spin state occurs through an absorption of a photon of radio-frequency (RF) energy RF Frequency of absorption: n = g Bo / 2 p

NMR Theory: Classical Description Spinning particle precesses around an applied magnetic field a) Angular velocity of this motion is given by: wo = g B o where the frequency of precession or Larmor frequency is: n = g. Bo/2 p Same as quantum mechanical description

Net Magnetization in a Magnetic Field z z Classic View: - Nuclei either align with or against external magnetic field along the z-axis. - Since more nuclei align with field, net magnetization (Mo) exists parallel to external magnetic field Mo x y Bo Bo Quantum Description: - Nuclei either populate low energy (a, aligned with field) or high energy (b, aligned against field) - Net population in a energy level. - Absorption of radiofrequency promotes nuclear spins from a b. b Bo > 0 DE = h n a Bo

An NMR Experiment We have a net magnetization precessing about Bo at a frequency of wo with a net population difference between aligned and unaligned spins. z z Mo x y Bo Bo Now What? Perturbed the spin population or perform spin gymnastics Basic principal of NMR experiments

The Basic 1 D NMR Experimental details will effect the NMR spectra and the corresponding interpretation

An NMR Experiment resonant condition: frequency (w 1) of B 1 matches Larmor frequency (wo) energy is absorbed and population of a and b states are perturbed. z Mo B 1 w 1 y z x B 1 off… (or off-resonance) x Mxy y w 1 And/Or: Mo now precesses about B 1 (similar to Bo) for as long as the B 1 field is applied. Again, keep in mind that individual spins flipped up or down (a single quanta), but Mo can have a continuous variation. Right-hand rule

Classical Description • Observe NMR Signal Ø Need to perturb system from equilibrium. § Ø Net magnetization (Mo) now precesses about Bo and B 1 § § § Ø B 1 field (radio frequency pulse) with g. Bo/2 p frequency MX and MY are non-zero Mx and MY rotate at Larmor frequency System absorbs energy with transitions between aligned and unaligned states Precession about B 1 stops when B 1 is turned off Mz RF pulse B 1 field perpendicular to B 0 Mxy

Absorption of RF Energy or NMR RF Pulse z Classic View: 90 o pulse - Apply a radio-frequency (RF) pulse a long the y-axis - RF pulse viewed as a second field (B 1), that the net magnetization (Mo) will precess about with an angular velocity of w 1 -- z Mo B 1 w 1 y x B 1 off… (or off-resonance) w 1 = g B 1 precession stops when B 1 turned off x Mxy y w 1 b Quantum Description: - enough RF energy has been absorbed, such that the population in a/b are now equal - No net magnetization along the z-axis DE = h n a Bo > 0 Please Note: A whole variety of pulse widths are possible, not quantized dealing with bulk magnetization

An NMR Experiment What Happens Next? The B 1 field is turned off and Mxy continues to precess about Bo at frequency wo. z x Mxy wo y Receiver coil (x) NMR signal FID – Free Induction Decay Mxy is precessing about z-axis in the x-y plane y Time (s) y y

An NMR Experiment The oscillation of Mxy generates a fluctuating magnetic field which can be used to generate a current in a receiver coil to detect the NMR signal. A magnetic field perpendicular to a circular loop will induce a current in the loop. NMR Probe (antenna)

NMR Signal Detection - FID The FID reflects the change in the magnitude of Mxy as the signal is changing relative to the receiver along the y-axis Detect signal along X RF pulse along Y Again, the signal is precessing about Bo at its Larmor Frequency (wo).

NMR Signal Detection - Fourier Transform So, the NMR signal is collected in the Time - domain But, we prefer the frequency domain. Fourier Transform is a mathematical procedure that transforms time domain data into frequency domain

NMR Signal Detection - Fourier Transform After the NMR Signal is Generated and the B 1 Field is Removed, the Net Magnetization Will Relax Back to Equilibrium Aligned Along the Z-axis T 2 relaxation Two types of relaxation processes, one in the x, y plane and one along the z-axis Peak shape also affected by magnetic field homogeneity or shimming

NMR Relaxation a) No spontaneous reemission of photons to relax down to ground state Probability too low cube of the frequency b) Two types of NMR relaxation processes spin-lattice or longitudinal relaxation (T 1) i. transfer of energy to the lattice or solvent material ii. coupling of nuclei magnetic field with magnetic fields created by the ensemble of vibrational and rotational motion of the lattice or solvent. iii. results in a minimal temperature increase in sample Mz = M 0(1 -exp(-t/T 1)) Recycle Delay: General practice is to wait 5 x. T 1 for the system to have fully relaxed.

NMR Relaxation spin-spin or transverse relaxation (T 2) i. exchange of energy between excited nucleus and low energy state nucleus ii. randomization of spins or magnetic moment in x, y-plane iii. related to NMR peak line-width Mx = My = M 0 exp(-t/T 2) (derived from Heisenberg uncertainty principal) Please Note: Line shape is also affected by the magnetic fields homogeneity

NMR Sensitivity The applied magnetic field causes an energy difference between aligned(a) and unaligned(b) nuclei b Bo > 0 Low energy gap DE = h n a Bo = 0 The population (N) difference can be determined from Boltzmman distribution: Na / Nb = e DE / k. T The DE for 1 H at 400 MHz (Bo = 9. 5 T) is 3. 8 x 10 -5 Kcal / mol Na / Nb = 1. 000064 Very Small ! ~64 excess spins per million in lower state

NMR Sensitivity NMR signal depends on: signal (s) ~ g 4 Bo 2 NB 1 g(u)/T 1) Number of Nuclei (N) (limited to field homogeneity and filling factor) 2) Gyromagnetic ratio (in practice g 3) 3) Inversely to temperature (T) 4) External magnetic field (Bo 2/3, in practice, homogeneity) 5) B 12 exciting field strength DE = g h Bo / 2 p Na / Nb = e DE / k. T Increase energy gap -> Increase population difference -> Increase NMR signal DE ≡ Bo ≡ g - Intrinsic property of nucleus can not be changed. g

NMR Sensitivity • Relative sensitivity of 1 H, 13 C, 15 N and other nuclei NMR spectra depend on Ø Gyromagnetic ratio (g) Ø Natural abundance of the isotope g - Intrinsic property of nucleus can not be changed. (g. H/g. C)3 1 H for 13 C is 64 x (g. H/g. N)3 for 15 N is 1000 x is ~ 64 x as sensitive as 13 C and 1000 x as sensitive as 15 N ! Consider that the natural abundance of 13 C is 1. 1% and 15 N is 0. 37% relative sensitivity increases to ~6, 400 x and ~2. 7 x 105 x !! 1 H NMR spectra of caffeine 8 scans ~12 secs 13 C NMR spectra of caffeine 10, 000 scans ~4. 2 hours

NMR Sensitivity Increase in Magnet Strength is a Major Means to Increase Sensitivity

NMR Sensitivity But at a significant cost! ~$800, 000 ~$2, 000 ~$4, 500, 000

Chemical Shift Up to this point, we have been treating nuclei in general terms. Simply comparing 1 H, 13 C, 15 N etc. If all 1 H resonate at 500 MHz at a field strength of 11. 7 T, NMR would not be very interesting The chemical environment for each nuclei results in a unique local magnetic field (Bloc) for each nuclei: Beff = Bo - Bloc --- Beff = Bo( 1 - s ) s is the magnetic shielding of the nucleus

Chemical Shift a) Small local magnetic fields (Bloc) are generated by electrons as they circulate nuclei. • Current in a circular coil generates a magnetic field b) These local magnetic fields can either oppose or augment the external magnetic field • Typically oppose external magnetic field • Nuclei “see” an effective magnetic field (Beff) smaller then the external field • s – magnetic shielding or screening constant i. depends on electron density ii. depends on the structure of the compound Beff = Bo - Bloc --- Beff = Bo( 1 - s )

Chemical Shift Beff = Bo - Bloc --- Beff = Bo( 1 - s ) HO-CH 2 -CH 3 s – reason why observe three distinct NMR peaks instead of one based on strength of B 0 n = g. Bo/2 p de-shielding high shielding Shielding – local field opposes Bo

Chemical Shift Effect of Magnetic Anisotropy 1) external field induces a flow (current) of electrons in p system – ring current effect 2) ring current induces a local magnetic field with shielding (decreased chemical shift) and deshielding (increased chemical shifts) Decrease in chemical shifts Increase in chemical shifts

The NMR scale (d, ppm) Bo >> Bloc -- MHz compared to Hz Comparing small changes in the context of a large number is cumbersome d= w - wref ppm (parts per million) Instead use a relative scale, and refer all signals (w) in the spectrum to the signal of a particular compound (wref). IMPORTANT: absolute frequency is field dependent (n = g Bo / 2 p) CH 3 Tetramethyl silane (TMS) is a common reference chemical H 3 C Si CH 3

The NMR scale (d, ppm) Chemical shift (d) is a relative scale so it is independent of Bo. Same chemical shift at 100 MHz vs. 900 MHz magnet IMPORTANT: absolute frequency is field dependent (n = g Bo / 2 p) At higher magnetic fields an NMR spectra will exhibit the same chemical shifts but with higher resolution because of the higher frequency range.

NMR Spectra Terminology TMS CHCl 3 7. 27 increasing d low field down field high frequency (u) de-shielding Paramagnetic 600 MHz 1 H 0 decreasing d high field up field low frequency high shielding diamagnetic 150 MHz 13 C ppm 92 MHz 2 H Increasing field (Bo) Increasing frequency (u) Increasing g Increasing energy (E, consistent with UV/IR)

Chemical Shift Trends For protons, ~ 15 ppm: For carbon, ~ 220 ppm: Carbon chemical shifts have similar trends, but over a larger sweep-width range (0 -200 ppm)

Chemical Shift Trends Acids Aldehydes Alcohols, protons a to ketones Aromatics Amides Olefins Aliphatic ppm 15 C=O in ketones 10 7 5 Aromatics, conjugated alkenes Olefins 2 0 TMS Aliphatic CH 3, CH 2, CH ppm 210 150 C=O of Acids, aldehydes, esters 100 80 50 0 TMS Carbons adjacent to alcohols, ketones

CHARACTERISTIC PROTON CHEMICAL SHIFTS Common Chemical Shift Ranges Carbon chemical shifts have similar trends, but over a larger sweep-width range (0200 ppm) Type of Proton Structure Chemical Shift, ppm Cyclopropane C 3 H 6 0. 2 Primary R-CH 3 0. 9 Secondary R 2 -CH 2 1. 3 Tertiary R 3 -C-H 1. 5 Vinylic C=C-H 4. 6 -5. 9 Acetylenic triple bond, CC-H 2 -3 Aromatic Ar-H 6 -8. 5 Benzylic Ar-C-H 2. 2 -3 Allylic C=C-CH 3 1. 7 Fluorides H-C-F 4 -4. 5 Chlorides H-C-Cl 3 -4 Bromides H-C-Br 2. 5 -4 Iodides H-C-I 2 -4 Alcohols H-C-OH 3. 4 -4 Ethers H-C-OR 3. 3 -4 Esters RCOO-C-H 3. 7 -4. 1 Esters H-C-COOR 2 -2. 2 Acids H-C-COOH 2 -2. 6 Carbonyl Compounds H-C-C=O 2 -2. 7 Aldehydic R-(H-)C=O 9 -10 Hydroxylic R-C-OH 1 -5. 5 Phenolic Ar-OH 4 -12 Enolic C=C-OH 15 -17 Carboxylic RCOOH 10. 5 -12 Amino RNH 2 1 -5

Coupling Constants through-bond interaction that results in the splitting of a single peak into multiple peaks of various intensities 1) The spacing in hertz (hz) between the peaks is a constant i. coupling constant (J) bonding electrons convey spin states of bonded nuclei 1) spin states of nuclei are “coupled” 2) alignment of spin states of bonded nuclei affects energy of the ground (a) and excited states (b) of observed nuclei 3) Coupling pattern and intensity follows Pascal’s triangle

Coupling Constants Energy level of a nuclei are affected by covalently-bonded neighbors spin-states 1 H 13 1 1 H H three-bond C one-bond Spin-States of covalently-bonded nuclei want to be aligned. +J/4 I J (Hz) bb S -J/4 ab ba S +J/4 I aa I S The magnitude of the separation is called coupling constant (J) and has units of Hz.

Coupling Constants 1 11 121 1331 14641 1 5 10 10 5 1 1 6 15 20 15 6 1 1 7 21 35 35 21 7 1

Common NMR Splitting Patterns Multiplets consist of 2 n. I + 1 lines I is the nuclear spin quantum number (usually 1/2) and n is the number of neighboring spins. singlet doublet 1: 1 triplet quartet 1: 2: 1 1: 3: 3: 1 pentet 1: 4: 6: 4: 1 Coupling Rules: 1. 2. 3. 4. 5. 6. equivalent nuclei do not interact coupling constants decreases with separation ( typically # 3 bonds) multiplicity given by number of attached equivalent protons (n+1) multiple spin systems multiplicity (na+1)(nb+1) Relative peak heights/area follows Pascal’s triangle Coupling constant are independent of applied field strength IMPORTANT: Coupling constant pattern allow for the identification of bonded nuclei.

Karplus Equation – Coupling Constants J = const. + 10 Cosf Relates coupling constant to Torsional angle. Used to solve Structures!

Example: The proton NMR spectrum is for a compound of empirical formula C 4 H 8 O. Identify the compound Absence of peak at ~9. 7 ppm eliminates aldehyde group And suggests ketone Triplet at ~1. 2 ppm suggests a methyl group coupled to a methylene group Strong singlet at ~2. 25 ppm methyl next to carbonyl Quartet at ~2. 5 ppm suggests a methylene next to a carbonyl coupled to a methyl

Nuclear Overhauser Effect (NOE) a) b) c) Interaction between nuclear spins mediated through empty space (#5Å) like ordinary bar magnets Important: effect is time-averaged Gives rise to dipolar relaxation (T 1 and T 2) and specially to cross -relaxation Perturb 1 H spin population affects 13 C spin population NOE effect

Nuclear Overhauser Effect (NOE) Nuclear Overhauser Effect (NOE, h) – the change in intensity of an NMR resonance when the transition of another are perturbed, usually by saturation. hi = (I-Io)/Io where Io is thermal equilibrium intensity Saturation – elimination of a population difference between transitions (irradiating one transition with a weak RF field) irradiate ab N A bb N-d X ba X aa N+d N A Populations and energy levels of a homonuclear AX system (large chemical shift difference) Observed signals only occur from single-quantum transitions

Nuclear Overhauser Effect (NOE) Saturated (equal population) ab N-½d S bb N-½d saturate I ba I aa N+½d S Saturated (equal population) Observed signals only occur from single-quantum transitions Populations and energy levels immediately following saturation of the S transitions ab W N-½d 1 A W 1 X bb N-½d W 2 W 0 aa N+½d W 1 X N+½d ba W 1 A Relaxation back to equilibrium can occur through: Zero-quantum transitions (W 0) Single quantum transitions (W 1) Double quantum transitions (W 2) The observed NOE will depend on the “rate” of these relaxation pathways

NMR Instrumentation (block diagram)

Superconducting Magnet a) solenoid wound from superconducting niobium/tin or niobium/titanium wire b) kept at liquid helium temperature (4 K), outer liquid N 2 dewar near zero resistance minimal current lose magnet stays at field for years without external power source Cross-section of magnet spinner sample lift NMR Tube RF coils cryoshims shimcoils Superconducting solenoid Use up to 190 miles of wire! Probe Liquid N 2 Liquid He

Superconducting Magnet a) Problems: Field drifts (B 0 changes) Remember: Field Drift over 11 Hrs (~ 0. 15 Hz/hr Field is not constant over sample (spatial variation) n = g. Bo/2 p

Lock System a) c) Corrects for magnetic field drift NMR probes contains an additional transmitter coil tuned to deuterium frequency changes in the intensity of the reference absorption signal controls a feedback circuit; a frequency generator provides a fixed reference frequency for the lock signal Lock Feedback Circuit if the observed lock signal differs from the reference frequency, a small current change occurs in a room-temperature shim coil (Z 0) to create a small magnetic field to augment the main field to place the lock-signal back into resonance Lock Changes From Off-resonance to Onresonance

Shim System a) c) Corrects for magnetic inhomogeneity Spatial arrangement of 20 coils actual shim coils Sketch of shim coils change current in each coil to “patch” differences in field and fix distortions in peak shape

Tune and Match System a) Tune- corrects the differences between observed and desired frequency correct impedance difference –Match c)between transmission resonant and circuit line (should be 50 W ) Adjust two capacitors until the tuning and desired frequency match and you obtain a null Affects: signal-to-noise accuracy of 90 o pulse sample heating chemical shift accuracy

Receiver Gain a) b) c) Amplifies the radio frequency FID signal from the probe Set to maximize signal-to-noise Signal is dependent on sample concentration The Analog to Digital Converter (ADC) has a maximum range of integers Clipped Fid Clipped FID Dynamic Range Problem

Continuous Wave (CW) vs. Pulse/Fourier Transform NMR Sensitivity Issue A frequency sweep (CW) to identify resonance is very slow (1 -10 min. ) Step through each individual frequency. Pulsed/FT collect all frequencies at once in time domain, fast (N x 1 -10 sec)

NMR Pulse a) In FT-NMR, how are all the individual nuclei excited simultaneously? b) RF pulses are typically short-duration (msecs) - produces bandwidth (1/4 t) centered around single frequency - shorter pulse width broader frequency bandwidth Heisenberg Uncertainty Principal: Du. Dt ~ 1/2 p A radiofrequency pulse is a combination of a wave (cosine) of frequency wo and a step function * = tp Pulse length (time, tp) The Fourier transform indicates the pulse covers a range of frequencies FT

NMR Pulse NMR pulse length or Tip angle (tp) z Mo z x qt tp x B 1 Mxy y y qt = g * t p * B 1 The length of time the B 1 field is on => torque on bulk magnetization (B 1) A measured quantity – instrument and sample dependent.

NMR Pulse Some useful common pulses z 90 o pulse Mo Maximizes signal in x, y-plane where NMR signal detected z x p/2 90 o y x Mxy y z 180 o pulse Inverts the spin-population. No NMR signal detected Mo z x y Can generate just about any pulse width desired. p 180 o x y -Mo

NMR Data Detection and Processing Fourier Transform NMR Increase signal-to-noise (S/N) by collecting multiple copies of FID and averaging signal. But, total experiment time is proportional to the number of scans time ~ (number of scans) x (recycle delay)

Proper Spectral Width Needs to be large enough to capture all the NMR resonances Correct Spectra with carrier offset resulting in peak folding or aliasing Sweep Width (range of radio-frequencies monitored for nuclei absorptions)

Digital Resolution – number of data points The FID is digitized Equal delay between points (dwell time) DT = 1 / (2 * SW) Want to maximize digital resolution, more data points increases acquisition time (AQ) and experimental time (ET): AQ = DT x NP ET = AQ x NS larger spectral width (SW) requires more data points for the same resolution

Digital Resolution – number of data points Want to maximize digital resolution:

Proper Acquisition Time Needs to be long enough to allow FID to Completely Decay Sinc Wiggles Truncated FID

Zero Filling Improve digital resolution by adding zero data points at end of FID 8 K data 8 K FID No zero-filling 8 K zero-fill 16 K FID 8 K zero-filling

Window Functions Emphasize the signal or decrease the noise by applying a mathematical function to the FID. Good stuff Mostly noise Sensitivity Resolution F(t) = 1 * e - ( LB * t ) – line broadening Effectively adds LB in Hz to peak Line-widths

Can either increase S/N or Resolution Not Both! LB = 5. 0 Hz Increase Sensitivity FT LB = -1. 0 Hz Increase Resolution FT

Baseline Correction Need a flat baseline – prefer to fix experimentally Apply any number of mathematical functions: linear Polynomial (upwards of 6 -orders) FID reconstruction Penalized parametric smoothing Etc. A number of factors lead to baseline distortions: Intense solvent or buffer peaks Phasing problems Errors in first data points of FID Short recycle tines Short acquisition times Receiver gain Xi & Roche BMC Bioinformatics (2008) 9: 234

Phase Correction Need a flat baseline – phase all peaks to be pure absorptive in shape Phase is due to difference in actual time and the zero-time point of FID (sin + cosines) Improper phasing can cause severe distortions in the baseline Xi & Roche BMC Bioinformatics (2008) 9: 234

NMR Peak Integration or Peak Area a) The relative peak intensity or peak area is proportional to the number of protons associated with the observed peak. b) Means to determine relative concentrations of multiple species present in an NMR sample. Relative peak areas = Number of protons 3 Integral trace HO-CH 2 -CH 3 1 2

Exchange Rates and NMR Time Scale i. Time Scale Slow Intermediate Fast Range (Sec-1) NMR time scale refers to the chemical shift time scale a) remember – frequency units are in Hz (sec-1) time scale b) exchange rate (k) c) differences in chemical shifts between species in exchange indicate the exchange rate. Chem. Shift (d) Coupling Const. (J) k << d. A- d. B k << JA- JB k = d. A - d. B k = JA- JB k >> d. A - d. B k >> JA- JB 0 – 1000 0 – 12 T 2 relaxation k << 1/ T 2, A- 1/ T 2, B k = 1/ T 2, A- 1/ T 2, B k >> 1/ T 2, A- 1/ T 2, B 1 - 20 d) For systems in fast exchange, the observed chemical shift is the average of the individual species chemical shifts. dobs = f 1 d 1 + f 2 d 2 f 1 +f 2 =1 where: f 1, f 2 – mole fraction of each species d 1, d 2 – chemical shift of each species

ii. Effects of Exchange Rates on NMR data k = p Dno 2 /2(he - ho) k = p Dno / 21/2 k = p (Dno 2 - Dne 2)1/2/21/2 k = p (he-ho) k – exchange rate h – peak-width at half-height n – peak frequency e – with exchange o – no exchange

NMR Dynamics and Exchange Equal Population of Exchange Sites No exchange: slow k = 0. 1 s-1 With exchange: Increasing Exchange Rate k = 5 s-1 k = 10 s-1 k = 20 s-1 k = 40 s-1 coalescence k = 88. 8 s-1 k = 200 s-1 k = 400 s-1 k = 800 s-1 fast k = 10, 000 s-1 40 Hz

Multidimensional NMR pulse sequences a) composed of a series of RF pulses, delays, gradient pulses and phases b) in a 1 D NMR experiment, the FID acquisition time is the time domain (t 1) c) more complex NMR experiments will use multiple “time-dimensional” to obtain data and simplify the analysis. d) Multidimensional NMR experiments may also use multiple nuclei (2 D, 13 C, 15 N) in addition to 1 H, but usually detect 1 H) 1 D NMR Pulse Sequence

Creating Multiple Dimensions in NMR a) collect a series of FIDS incremented by a second time domain (t 1) b) the normal acquisition time is t 2. c) Fourier transformation occurs for both t 1 and t 2, creating a twodimensional (2 D) NMR spectra Relative appearance of each NMR spectra will be modulated by the t 1 delay

Creating Multiple Dimensions in NMR In 2 D NMR spectra, diagonal peaks are normal 1 D peaks, off-diagonal or crosspeaks indicate a correlation between the two diagonal peaks Collections of FIDs with t 1 modulations Fourier Transform t 1 obtain 2 D NMR spectra Fourier Transform t 2 obtain series of NMR spectra modulated by t 1 Looking down t 1 axis, each point has characteristics of time domain FID Peaks along diagonal are normal 1 D NMR spectra Contour map (slice at certain threshold) of 3 D representation of 2 D NMR spectra. (peak intensity is third dimension Cross-peaks correlate two diagonal peaks by J-coupling or NOE interactions

2 D 1 H-1 H NOESY Experiment Diagonal peaks are correlated by through-space dipole-dipole interaction (NOE) Relative magnitude of cross-peak is related to distance (1/R 6) between protons (≥ 5Å) Diagonal peaks corresponds to 1 D NMR spectra Cross peaks correlate diagonal peaks by NOEs

2 D 1 H-13 C HSQC Experiment Correlates all directly bonded 13 C-1 H pairs generally requires 13 C-labeling (1. 1% natural abundance)

2 D 1 H-1 H TOCSY Experiment Correlates all 3 -bonded 1 H-1 H pairs in a molecules

3 D & 4 D NMR Spectra a) additional dimensions usually correspond to 13 C & 15 N chemical shifts. b) primarily used for analysis of biomolecular structures - disperses highly overlapped NMR spectra into 3 D & 4 D c) view 3 D, 4 D experiments as collection of 2 D spectra. d) one experiment may take 2. 5 to 4 days to collect. Spread peaks out by 15 N chemical shift of amide N attached to NH Further spread peaks out by 13 C chemical shift of C attached to CH