a. s. edison university of florida 2006 today’s lecture 13) mon, oct 30: assignments: i a....
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A. S. EdisonUniversity of Florida2006
Today’s Lecture
13) Mon, Oct 30: Assignments: Ia. Important homonuclear (e.g. 1H)
experimentsb. Small moleculesc. Peptide assignments
A. S. EdisonUniversity of Florida2006
Homonuclear 2D ExperimentsName Type of correlation Notes
COSY Correlated Spectroscopy
1H atoms separated by 2 or 3 covalent bonds and mediated by J-coupling (sometimes up to 5 bonds). Several variants available.
Only pairs of coupled atoms (compare to TOCSY). Cross peaks antiphase.
TOCSY Total Correlation Spectroscopy
1H atoms separated by 2 or 3 covalent bonds and mediated by J-coupling. All 1H in a network of coupled spins will be correlated
Correlations between networks of coupled spins. Very useful for side-chains in peptides/proteins. Cross peaks in phase.
NOESY Nuclear Overhauser Effect Spectroscopy
1H atoms up to ~5 Å in space mediated by dipolar interactions. The NOE is highly dependent on molecular correlation time: Small molecules have positive NOE and large molecules are negative. Larger molecules have faster transfer rates. Intermediate sized molecules (~500 Da) do not work with NOESY.
Crude but important measure of atomic distances; generally categorize into “strong” (<2.5 Å), “medium” (<4 Å), “weak” (>4 Å). Spin diffusion can cause problems in accurate measurements.
ROESY Rotating Frame Overhauser Effect Spectroscopy
1H atoms up to ~5 Å in space mediated by dipolar interactions. Unlike NOESY, ROESY is the same sign regardless of correlation time. This is especially useful for intermediate MW where NOESY doesn’t work.
ROESY uses a transverse spin lock and is very similar to TOCSY. For this reason, ROESY experiments often have more artifacts than NOESY.
A. S. EdisonUniversity of Florida2006
DQF-COSY: Double quantum filtered COSY to clean up diagonal and reduce solvent
Dossey, A. T., Walse, S. S., Rocca, J. R., & Edison, A. S. “Single Insect NMR: A New Tool to Probe Chemical Biodiversity” ACS Chemical Biology, 1 (8), 511–514 (2006).
A. S. EdisonUniversity of Florida2006
TOCSY: 60 ms DIPSI-2 mixing time
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ROESY: 400 ms cw mixing time
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TOCSY and COSY comparison
A. S. EdisonUniversity of Florida2006
ROESY and COSY comparison
A. S. EdisonUniversity of Florida2006
TOCSY OVERVIEW
•TOCSY (Total Correlation Spectroscopy) is capable of correlating all spins in a coupled network (examples shown on the next slide).
•The “working end” of the TOCSY pulse sequence is an isotropic mixing sequence that is a sequence of pulses that are designed to remove all chemical shift differences and create a strong coupling environment. This is called the Hartmann-Hahn condition. Sometimes the TOCSY experiment is called HOHAHA (Homonuclear Hartmann-Hahn).
•Several mixing sequencings have been developed. The most popular are MLEV-17, WALTZ-16, GARP, and DIPSI. These all apply a series of pulses with either different phases or different lengths or both.
•The strong coupling product operator is similar to the regular (weak) coupling operator but it includes IxSx and IySy terms.
•The net result of the TOCSY mixing sequence is the transfer of magnetization from I to S along the same axis (e.g. Iz to Sz or Ix to Sx or Iy to Sy). The transfer depends on the coupling constant but is fairly complicated because S can transfer to another spin, R, and so on.
A. S. EdisonUniversity of Florida
A. S. EdisonUniversity of Florida2006
TOCSY Pulse sequence
(the simplest of several variants)
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90x
t1 Isotropic Mixing
MLEV-17: (90-y, 180x, 90-y, 90-y, 180x, 90-y)*n 60x
DIPSI-2: (320, 410, 290, 285, 30, 245, 375, 265, 370)*n
The numbers are pulse lengths in degrees. The red and black pulses are 180 degrees out of phase. The element in the parenthesis is repeated n-times to get the desired mixing time (e.g. 20-80 ms)
A. S. EdisonUniversity of Florida2006
Spin Systems
CH3
CH3CH3
H H H H H H
H H H H
H
Any set of protons in a chain of unbroken J-coupling interactions will
give rise to sets of TOCSY cross peaks. For example, each of the 3 sets
of peaks shown above will be correlated in a 2D TOCSY spectrum.
A. S. EdisonUniversity of Florida
A. S. EdisonUniversity of Florida2006
TOCSY spectrum of a 16 amino acid peptide
H2
H1
1357
1
3
5
7
9
Each amino acid will produce
a pattern of peaks that
represent the network of
coupled spins in that amino
acid. The highlighted spin
system shown in red is a
leucine. Note that there are
two leucines with very similar
chemical shifts.
A. S. EdisonUniversity of Florida
Zachariah, C., Cameron, A., Lindberg, I., Kao, K. J., Beinfeld, M. C., and Edison, A. S. “Structural Studies of a Neuropeptide Precursor Protein with an RGD Proteolytic Site” Biochemistry 40, 8790-8799 (2001).
A. S. EdisonUniversity of Florida2006
NOE
•Transferring magnetization through scalar coupling is a “coherent” process. This means that all of the spins are doing the same thing at the same time.
•Relaxation is an “incoherent” process, because it is caused by random fluxuations that are not coordinated.
•The nuclear Overhauser effect (NOE) is in incoherent process in which two nuclear spins “cross-relax”. Recall that a single spin can relax by T1 (longitudinal or spin-latice) or T2 (transverse or spin-spin) mechanisms. Nuclear spins can also cross-relax through dipole-dipole interactions and other mechanisms. This cross relaxation causes changes in one spin through perturbations of the other spin.
•The NOE is dependent on many factors. The major factors are molecular tumbling frequency and internuclear distance. The intensity of the NOE is proportional to r-6 where r is the distance between the 2 spins.
A. S. EdisonUniversity of Florida
A. S. EdisonUniversity of Florida2006
A. S. EdisonUniversity of Florida
NOE vs. ROE
NOE goes through zero c
NOE
Small peptides ~10 kDa ~33kDa
Enh
ance
men
t
A. S. EdisonUniversity of Florida2006
A. S. EdisonUniversity of Florida
NOESY pulse sequence
A. S. EdisonUniversity of Florida
90
t1
90 90
Like all 2D sequences, t1 is the variable time to collect frequency information in the indirect dimension. The delay is fixed and is the time during which the NOE builds up. You might have guessed that chemical exchange can also happen during this time, and it is possible to confuse an NOE peak with a chemical exchange peak, but techniques have been developed to figure out which is which.
Notice that I have not indicated the phases of the pulses. The different ’s make up a phase-cycle, and we can also adjust which axis from which to record the signal (rec). These are designed to minimize artifacts and select for desired correlations. Most 2D pulse sequences have phase cycles.
rec
A. S. EdisonUniversity of Florida2006
NOESY and TOCSY spectra of a 16 amino acid peptide
Each cross peak in a NOESY spectrum indicates that the nuclei resonating at the 2 frequencies are within 5 Å in space.
H2
H1
1357
1
3
5
7
9
Notice the difference between TOCSY (black) and NOESY (red).
A. S. EdisonUniversity of Florida2006
TOCSY/COSY
NOESY/ROESY
1H-based Peptide Resonance Assignments
NC
C’N
CC’
H O
H OHCH3
HCH
CH3CH3
N
H
A. S. EdisonUniversity of Florida2006
1H-based Resonance Assignments
F2
G3
E5
G10
M6
M8
F14
V11
D4
L12
R13
"NH"2
8.7 8.4 8.1 7.8ppm
4.8
4.5
4.2
3.9
GFGDEMSMPGVLRFamide
S7
A. S. EdisonUniversity of Florida2006
Next Lecture
A. S. EdisonUniversity of Florida
14) Wed, Nov 1: Assignments: II
a.Important heteronuclear experiments
b.3D NMR
c.Assignment strategies in proteins
d.Intro to protein structure determination