Difference: EinsteinSyllabus (1 vs. 2)

Revision 203 Nov 2006 - Main.DavidCowburn

 
META TOPICPARENT name="NmrEducation"
Biochemical Applications of NMR Spectroscopy (AECOM, 1998 - present)

*Introduction*

1. Introduction

Changed:
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<
General overview of NMR and its applications in biochemistry Overview of the course
>
>
  1. General overview of NMR and its applications in biochemistry
  2. Overview of the course
 2. Basic Principles of NMR
Changed:
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Nuclear spin (I): who's got it, and how much Magnetic moment (m & g). Isolated spin in a magnetic field B0, torque, and w0. E, DE, Boltzman (and g) The basic NMR experiment: B1 (R.F.) and resonance The rotating frame The experiment: delay, pulse, observe Application of a pulse Effect Flip angle Description of signal (intensity, frequency, decay) The Fourier Transform (FT) Summary
>
>
  1. Nuclear spin (I): who's got it, and how much
  2. Magnetic moment (m & g).
  3. Isolated spin in a magnetic field
  4. B0, torque, and w0.
  5. E, DE, Boltzman (and g)
  6. The basic NMR experiment:
    1. B1 (R.F.) and resonance
    2. The rotating frame
    3. The experiment: delay, pulse, observe
    4. Application of a pulse
    5. Effect
    6. Flip angle
    7. Description of signal (intensity, frequency, decay)
    8. The Fourier Transform (FT)
  7. Summary
  3. Signal properties & data processing
Changed:
<
<
Review R.F. Pulse brings magnetization into transverse (x,y) plane. Magnetization precesses at (w0+wi) Rotating frame (and the "carrier" + "offset") Free Induction Decay (FID), oscillates at wi Mathematical description Iz, Ix, Iy: components of magnetization (projections) along z, x, & y axes Start with Iz=unity, Ix=0, Iy=0. (normalized; actual magnetization M depends on # spins, gamma, and B0) Pulse rotates Iz through flip angle a around axis of pulse
>
>
  1. Review
    1. .F. Pulse brings magnetization into transverse (x,y) plane.
    2. Magnetization precesses at (w0+wi)
    3. Rotating frame (and the "carrier" + "offset")
    4. Free Induction Decay (FID), oscillates at wi
    5. Mathematical description
      1. Iz, Ix, Iy: components of magnetization (projections) along z, x, & y axes
      2. Start with Iz=unity, Ix=0, Iy=0. (normalized; actual magnetization M depends on # spins, gamma, and B0)
      3. Pulse rotates Iz through flip angle a around axis of pulse
  e.g. a along y axis: aÎy (again = gB1t)
Changed:
<
<
Result
Izcos(a) + Ixsin(a). If a=90 , then simply have Ix, since cos(90)=0, sin(90)=1 With time (t), magnetization precesses in the x,y plane. This is the same as a rotation about the z axis of angle (wt). i.e. (wt)Îz So the signal (FID) can be described as: Ixcos(wt) + Iysin(wt) It decays in the x,y plane with a time constant T2 as exp(-t/T2): Ixcos(wt)exp(-t/T2) + Iysin(wt)exp(-t/T2) Can also write as complex exponential exp(iwt-t/T2) Sampled signal Use "quadrature detection" to observe the signal, and determine sign of precession relative to carrier Results in a "complex" signal (Ix + iIy) Discretely sampled Sampling rate: Dt or "dwell time" (DW). Nyquist theorem Spectral width (SW) in Hz = 1/(2Dt) Folding or aliasing The discrete fourier transform (DFT)
>
>
      1. Result: Izcos(a) + Ixsin(a). If a=90 , then simply have Ix, since cos(90)=0, sin(90)=1
    1. With time (t), magnetization precesses in the x,y plane.
      1. This is the same as a rotation about the z axis of angle (wt). i.e. (wt)Îz
      2. So the signal (FID) can be described as:
      3. Ixcos(wt) + Iysin(wt)
      4. It decays in the x,y plane with a time constant T2 as exp(-t/T2):
      5. Ixcos(wt)exp(-t/T2) + Iysin(wt)exp(-t/T2)
      6. Can also write as complex exponential exp(iwt-t/T2)
    2. Sampled signal
      1. Use "quadrature detection" to observe the signal, and determine sign of precession relative to carrier
      2. Results in a "complex" signal (Ix + iIy)
      3. Discretely sampled
      4. Sampling rate: Dt or "dwell time" (DW).
      5. Nyquist theorem
      6. Spectral width (SW) in Hz = 1/(2Dt)
      7. Folding or aliasing
    3. The discrete fourier transform (DFT)
Added:
>
>
  Formula "Real" absorptive Lorentzian + "imaginary" dispersive Lorentzian signals (only look at absorptive) Linewidth & T2 Digital resolution Number of data points (TD) & noise Zero Filling (SI) Linear Prediction Window or apodization functions Truncation artifacts Exponential (EM) Matched filter Gaussian (GM) Sine bell (SB) Phase and phasing Origin of phase errors Receiver and transmitter phase errors: frequency independent (zero order) Initial sampling delay: frequency dependent (first order) Zero and first order correction procedure Signal & Noise Definition of signal to noise (S/N) Signal averaging Number of scans (NS) S/N proportional to (NS)1/2 Putting it all together for the 1D experiment: Relaxation delay , Pulse, Acquire Text file for pulse program Setup (ased) Pulse length (p1), relaxation delay (d1), SW, TD, SI, NS, O1, RG Acquire (ZG) Window (LB, EM) FT Phase
Preview
NMR spectral parameters: chemical shift, coupling, T1, T2

4. Chemical shift & spin-spin coupling; Introduction to T1 and T2.

Chemical Shift Definition (B_local, shielding constant = sigma) Field dependant (a reason for going to larger magnets - better resolution) Field independent units: ppm Reference standards Indirect referencing JACS 106, 1939-1941 (1984); J. Biomol. NMR 6, 135-50 (1995) Ranges for 1H 13C 31P 19F 15N Origins: Intrinsic ("chemical") Electron density Diamagnetic and paramagnetic components Extrinsic ("environmental") Ring current (also carbonyls, etc) Leads to conformation-dependent chemical shifts in macromolecules

Note
old scales and sign conventions Example uses of chemical shifts: Ionization states Protein secondary structure Stereochemistry Isotope shifts and reaction mechanisms Hydrogen bonds

Spin-spin coupling, two kinds. Dipolar Large, normally averaged out in solution But - relatively recent work at high field (Tjandra & Bax Science 278,1111 1997)

Spin-spin coupling through bonding electrons

Multiplicities
2nI+1 Weak vs strong coupling Typical values Field independent
Nomenclature
nJAB, AMX
  1. , 2, & 3 bond Ranges for 1H, 13C, 15N, 31P Dependence on dihedral angle (Karplus) Use in assignments (Decoupling, and coherence transfer)

Relaxation - linewidth in spectrum, and intensity vs. relaxation delay

T1
relaxation towards thermal equilibrium Qualitative description and overview of measurement

T2
relaxation in the transverse plane. Qualitative description and overview of measurement Both depend on molecular motion

Lab 1: Introduction & basic 1D experiment

*Basic Experiments & Small Molecules*

5. Relaxation & the NOE

6. Product operator description & coherence transfer

7. A repertoire of one-dimensional methods Review of the basic 1D experiment (zg, zg30) - note: phase cycle Broadband decoupling (zgdc, zgdc30; BAUG pp. 37-40) Homonuclear gated decoupling (zghd) Solvent suppression Why work in 1H solvent? Presaturation (zgpr) Gradient methods Introduction to gradients Selective pulses (selzg; BAUG pp. 83-100) Watergate (p3919gp) Jump and return, a.k.a. 1:1 (p11) T1 - inversion recovery (t1ir; BAUG pp. 71-81) T2 - spin echo, Carr-Purcell-Meiboom-Gill (cpmg) Steady-state NOE Homonuclear - NOE difference (noedif) Heteronuclear Transient NOE Initial rate approximation Distances TOE (noedif; BAUG pp. 101-111) Heteronuclear coherence transfer: DEPT (dept; BAUG pp. 65-70) Doddrell et al, J. Magn. Reson. 48, 323 (1982) Signal to noise enhancement Spectral editing

Lab 2: 1D homonuclear and heteronuclear experiments

8. Introduction to two-dimensional NMR Building blocks: INEPT reverse INEPT INEPT-revINEPT, as a filter The second dimension, via the HSQC (INEPT-t1-reverse INEPT) Quadrature in t1 Practical issues

9. 2D Heteronuclear experiments

10. 2D Homonuclear experiments Introduction The three most important homonuclear experiments: COSY - cross peaks between protons <= 3 bonds apart TOCSY - cross peaks from all members of a spin system NOESY - cross peaks from through-space dipolar coupling COSY & TOCSY - assignment of resonances NOESY - conformation (distances between assigned spins) Together provide sufficient data to determine the complete structures of small proteins and nucleic acids - important experiments indeed.

COSY
COrrelation SpectroscopY? Aue, Bartoli, & Ernst J. Chem. Phys. 64, 2229-46 (1976) First 2D experiment ever proposed (1971) Cross peaks from scalar coupled 1H <= 3 bonds apart. Example spectrum (R2-CH-CH2-CH3) Pulse sequence: ____|___t1___| \/\/\/\/\/\/\/\/ Looks simple, but - Results of product operator analysis
Note
here both I and S are protons Start on Iz as usual
  1. Îx -> -Iy During t1, both chemical shift evolution (wt1Îz) and coupling (pJt1Î1zÎ2z) I->S transfer builds up over t1 as sin(pJt1) ¿ so no cross peak signal in initial FIDs Terms leading to diagonal and cross peaks Properties of cross-peak and diagonal Diagonal - in-phase doublet Cross peaks - anti-phase doublet The two are 90 degrees out of phase with each other Can get cancellation in cross peaks for molecules with large linewidths

Examples

Variant
DQF-COSY - Double Quantum Filtered COSY Rance et al, BBRC 117, 479-485 (1983) Pulse sequence: ___|__t1__| | \/\/\/\/\/\/\/\/ Final pulse converts MQ term in COSY into observable magnetization Diagonal and cross peaks simultaneously in phase Reduced contributions from "peaks without partners" - e.g. H2O But, lose factor of 2 in signal Usually worth the tradeoff & this is the standard COSY experiment Processing, phasing Final Note: caution about coupling constants from COSY Mutual cancellation and distortion. (E. COSY: "Exclusive COSY") Resonance overlap - a problem even in 2D NMR (example). A helpful experiment is: .... and so on for:
TOCSY
TOtal Correlation SpectroscopY? (a.k.a. "HOHAHA") NOESY (via the Transient 1D NOE) ROESY EXSY

Lab 3: 2D Correlation experiments

11. Pulsed field gradients, Solvent suppression, and Selfdiffusion

*Macromolecular Structure*

Small Proteins and Nucleic Acids

12. Resonance assignments

14. Structural Constraints

Lab 4: 23 residue antibiotic peptide: 2D correlation spectra & assignments

15. Structure calculation & refinement

16. Structure evaluation

17. Nucleic Acids: assignments, constraints & structure

Lab 5: 2D NOESY spectrum & analysis

18. Representative protein and nucleic acid NMR structure determinations

19. Conformation of ligands on macromolecules

Lab 6: Structure calculation & analysis

Larger Proteins & Nucleic Acids - Isotopic labeling & 3D experiments

20. Introduction to 3D NMR (via NOESY-HSQC and TOCSY-HSQC)

21. Triple resonance experiment and stucture determination, Part I

Lab7: 2D & 3D 1H15N spectra of labeled proteins

22. Triple resonance experiments and stucture determination, Part II ... including labeling, deuteration, and example 3D structure determination

23. On to larger (> 30kD) proteins

*Biochemical Applications*

Ligands, Kinetics & Mechanism

24. Water & hydrogen bonds

25. Ionization states & pK_a's

Lab 8: Triple resonance experiments

26. NMR-Based Screening in Drug Discovery

27. "Fun with Enzymes": k_on, k_off, K_eq, K_eq', PIX, etc.

28. Folding of proteins & nucleic acids

Lab 9: Titration of histidine pK_a's in ribonuclease

*Dynamics*

29. Metabolic studies in cells

30. Exchange & measuring dynamic processes

Lab 10: Substrate k_on and k_off from saturation transfer

31. Heteronuclear relaxation & Macromolecular dynamics

Revision 103 Nov 2006 - Main.DavidCowburn

 
META TOPICPARENT name="NmrEducation"
Biochemical Applications of NMR Spectroscopy (AECOM, 1998 - present)

*Introduction*

1. Introduction General overview of NMR and its applications in biochemistry Overview of the course

2. Basic Principles of NMR Nuclear spin (I): who's got it, and how much Magnetic moment (m & g). Isolated spin in a magnetic field B0, torque, and w0. E, DE, Boltzman (and g) The basic NMR experiment: B1 (R.F.) and resonance The rotating frame The experiment: delay, pulse, observe Application of a pulse Effect Flip angle Description of signal (intensity, frequency, decay) The Fourier Transform (FT) Summary

3. Signal properties & data processing Review R.F. Pulse brings magnetization into transverse (x,y) plane. Magnetization precesses at (w0+wi) Rotating frame (and the "carrier" + "offset") Free Induction Decay (FID), oscillates at wi Mathematical description Iz, Ix, Iy: components of magnetization (projections) along z, x, & y axes Start with Iz=unity, Ix=0, Iy=0. (normalized; actual magnetization M depends on # spins, gamma, and B0) Pulse rotates Iz through flip angle a around axis of pulse e.g. a along y axis: aÎy (again = gB1t)

Result
Izcos(a) + Ixsin(a). If a=90 , then simply have Ix, since cos(90)=0, sin(90)=1 With time (t), magnetization precesses in the x,y plane. This is the same as a rotation about the z axis of angle (wt). i.e. (wt)Îz So the signal (FID) can be described as: Ixcos(wt) + Iysin(wt) It decays in the x,y plane with a time constant T2 as exp(-t/T2): Ixcos(wt)exp(-t/T2) + Iysin(wt)exp(-t/T2) Can also write as complex exponential exp(iwt-t/T2) Sampled signal Use "quadrature detection" to observe the signal, and determine sign of precession relative to carrier Results in a "complex" signal (Ix + iIy) Discretely sampled Sampling rate: Dt or "dwell time" (DW). Nyquist theorem Spectral width (SW) in Hz = 1/(2Dt) Folding or aliasing The discrete fourier transform (DFT) Formula "Real" absorptive Lorentzian + "imaginary" dispersive Lorentzian signals (only look at absorptive) Linewidth & T2 Digital resolution Number of data points (TD) & noise Zero Filling (SI) Linear Prediction Window or apodization functions Truncation artifacts Exponential (EM) Matched filter Gaussian (GM) Sine bell (SB) Phase and phasing Origin of phase errors Receiver and transmitter phase errors: frequency independent (zero order) Initial sampling delay: frequency dependent (first order) Zero and first order correction procedure Signal & Noise Definition of signal to noise (S/N) Signal averaging Number of scans (NS) S/N proportional to (NS)1/2 Putting it all together for the 1D experiment: Relaxation delay , Pulse, Acquire Text file for pulse program Setup (ased) Pulse length (p1), relaxation delay (d1), SW, TD, SI, NS, O1, RG Acquire (ZG) Window (LB, EM) FT Phase
Preview
NMR spectral parameters: chemical shift, coupling, T1, T2

4. Chemical shift & spin-spin coupling; Introduction to T1 and T2.

Chemical Shift Definition (B_local, shielding constant = sigma) Field dependant (a reason for going to larger magnets - better resolution) Field independent units: ppm Reference standards Indirect referencing JACS 106, 1939-1941 (1984); J. Biomol. NMR 6, 135-50 (1995) Ranges for 1H 13C 31P 19F 15N Origins: Intrinsic ("chemical") Electron density Diamagnetic and paramagnetic components Extrinsic ("environmental") Ring current (also carbonyls, etc) Leads to conformation-dependent chemical shifts in macromolecules

Note
old scales and sign conventions Example uses of chemical shifts: Ionization states Protein secondary structure Stereochemistry Isotope shifts and reaction mechanisms Hydrogen bonds

Spin-spin coupling, two kinds. Dipolar Large, normally averaged out in solution But - relatively recent work at high field (Tjandra & Bax Science 278,1111 1997)

Spin-spin coupling through bonding electrons

Multiplicities
2nI+1 Weak vs strong coupling Typical values Field independent
Nomenclature
nJAB, AMX
  1. , 2, & 3 bond Ranges for 1H, 13C, 15N, 31P Dependence on dihedral angle (Karplus) Use in assignments (Decoupling, and coherence transfer)

Relaxation - linewidth in spectrum, and intensity vs. relaxation delay

T1
relaxation towards thermal equilibrium Qualitative description and overview of measurement

T2
relaxation in the transverse plane. Qualitative description and overview of measurement Both depend on molecular motion

Lab 1: Introduction & basic 1D experiment

*Basic Experiments & Small Molecules*

5. Relaxation & the NOE

6. Product operator description & coherence transfer

7. A repertoire of one-dimensional methods Review of the basic 1D experiment (zg, zg30) - note: phase cycle Broadband decoupling (zgdc, zgdc30; BAUG pp. 37-40) Homonuclear gated decoupling (zghd) Solvent suppression Why work in 1H solvent? Presaturation (zgpr) Gradient methods Introduction to gradients Selective pulses (selzg; BAUG pp. 83-100) Watergate (p3919gp) Jump and return, a.k.a. 1:1 (p11) T1 - inversion recovery (t1ir; BAUG pp. 71-81) T2 - spin echo, Carr-Purcell-Meiboom-Gill (cpmg) Steady-state NOE Homonuclear - NOE difference (noedif) Heteronuclear Transient NOE Initial rate approximation Distances TOE (noedif; BAUG pp. 101-111) Heteronuclear coherence transfer: DEPT (dept; BAUG pp. 65-70) Doddrell et al, J. Magn. Reson. 48, 323 (1982) Signal to noise enhancement Spectral editing

Lab 2: 1D homonuclear and heteronuclear experiments

8. Introduction to two-dimensional NMR Building blocks: INEPT reverse INEPT INEPT-revINEPT, as a filter The second dimension, via the HSQC (INEPT-t1-reverse INEPT) Quadrature in t1 Practical issues

9. 2D Heteronuclear experiments

10. 2D Homonuclear experiments Introduction The three most important homonuclear experiments: COSY - cross peaks between protons <= 3 bonds apart TOCSY - cross peaks from all members of a spin system NOESY - cross peaks from through-space dipolar coupling COSY & TOCSY - assignment of resonances NOESY - conformation (distances between assigned spins) Together provide sufficient data to determine the complete structures of small proteins and nucleic acids - important experiments indeed.

COSY
COrrelation SpectroscopY? Aue, Bartoli, & Ernst J. Chem. Phys. 64, 2229-46 (1976) First 2D experiment ever proposed (1971) Cross peaks from scalar coupled 1H <= 3 bonds apart. Example spectrum (R2-CH-CH2-CH3) Pulse sequence: ____|___t1___| \/\/\/\/\/\/\/\/ Looks simple, but - Results of product operator analysis
Note
here both I and S are protons Start on Iz as usual
  1. Îx -> -Iy During t1, both chemical shift evolution (wt1Îz) and coupling (pJt1Î1zÎ2z) I->S transfer builds up over t1 as sin(pJt1) ¿ so no cross peak signal in initial FIDs Terms leading to diagonal and cross peaks Properties of cross-peak and diagonal Diagonal - in-phase doublet Cross peaks - anti-phase doublet The two are 90 degrees out of phase with each other Can get cancellation in cross peaks for molecules with large linewidths

Examples

Variant
DQF-COSY - Double Quantum Filtered COSY Rance et al, BBRC 117, 479-485 (1983) Pulse sequence: ___|__t1__| | \/\/\/\/\/\/\/\/ Final pulse converts MQ term in COSY into observable magnetization Diagonal and cross peaks simultaneously in phase Reduced contributions from "peaks without partners" - e.g. H2O But, lose factor of 2 in signal Usually worth the tradeoff & this is the standard COSY experiment Processing, phasing Final Note: caution about coupling constants from COSY Mutual cancellation and distortion. (E. COSY: "Exclusive COSY") Resonance overlap - a problem even in 2D NMR (example). A helpful experiment is: .... and so on for:
TOCSY
TOtal Correlation SpectroscopY? (a.k.a. "HOHAHA") NOESY (via the Transient 1D NOE) ROESY EXSY

Lab 3: 2D Correlation experiments

11. Pulsed field gradients, Solvent suppression, and Selfdiffusion

*Macromolecular Structure*

Small Proteins and Nucleic Acids

12. Resonance assignments

14. Structural Constraints

Lab 4: 23 residue antibiotic peptide: 2D correlation spectra & assignments

15. Structure calculation & refinement

16. Structure evaluation

17. Nucleic Acids: assignments, constraints & structure

Lab 5: 2D NOESY spectrum & analysis

18. Representative protein and nucleic acid NMR structure determinations

19. Conformation of ligands on macromolecules

Lab 6: Structure calculation & analysis

Larger Proteins & Nucleic Acids - Isotopic labeling & 3D experiments

20. Introduction to 3D NMR (via NOESY-HSQC and TOCSY-HSQC)

21. Triple resonance experiment and stucture determination, Part I

Lab7: 2D & 3D 1H15N spectra of labeled proteins

22. Triple resonance experiments and stucture determination, Part II ... including labeling, deuteration, and example 3D structure determination

23. On to larger (> 30kD) proteins

*Biochemical Applications*

Ligands, Kinetics & Mechanism

24. Water & hydrogen bonds

25. Ionization states & pK_a's

Lab 8: Triple resonance experiments

26. NMR-Based Screening in Drug Discovery

27. "Fun with Enzymes": k_on, k_off, K_eq, K_eq', PIX, etc.

28. Folding of proteins & nucleic acids

Lab 9: Titration of histidine pK_a's in ribonuclease

*Dynamics*

29. Metabolic studies in cells

30. Exchange & measuring dynamic processes

Lab 10: Substrate k_on and k_off from saturation transfer

31. Heteronuclear relaxation & Macromolecular dynamics

 
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