Title: Protein NMR: Assignment Structure Dynamics
1Protein NMRAssignment Structure Dynamics
2- Cross peak proof of J coupling, i.e. of a bond
3Double Fourier Transformation
4Fourier Transformation
5The J doublet
- Each member of the doublet is treated as a
separate magnetization vector, with its own
precession rate. - Note that the passive spin is in a discrete
quantum state up or down, but never in between.
(Stern Gerlach).
6Transfer of magnetization in the J doublet
- Initial state proton polarization or population
difference follows its Boltzmann factor for its
energy difference, and nitrogen follows its
population difference follows its Boltzmann
factor for its energy difference - Final State nitrogen polarization or population
difference follows the Boltzmann factor for its
energy difference for protons 10z stronger mag
vector!
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8Selective Inversions
- Selective Inversion of one line in the doublet
without touching the other can be accomplished
in two very different ways. - 1) 90 - precession until antiphase -90
- 2) weak irradiation on resonance for one line
- 1) Can be accomplished for many frequencies
(chemica shift values) simultaneously
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10HSQC
- Standard fingerprint
- Folded proteins give nicely dispersed spectra
(each a.a. is shifted to a unique frequency)
BOTTOM 2D 15N 1H. Empirical rules distinguish
sheet and helix and coil (somewhat) - Unfolded proteins in solution give non-dispersed
lines TOP - Data from Dr. Cheryl Arrowsmith, U. Toronto
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123D spectroscopy
Ni Cai COi,/ Cbi
Ni CO i-1 Ca i-1
13Protein Spectra Multinuclear and Site Specific
- Slice the cube at a particular 15N frequency
- Strip along a particular 1H frequency
- The 1H-15N pair of frequencies is already
identified from the HSQC fingerprint - Learn the 13C frequencies for Ca and Cb
14Relaxation
15How we measure relaxation
16Simple Sequence for T1 Inversion Recovery
17Simple Sequence for T2 Echo
18Case 1 Neigboring Nucleus is high energy
Splittings are due to Quantized Neighbors
S
Field due to neighbor
Applied Field
Case 2 Neigboring Nucleus is low energy
N
Field due to neighbor
19Relaxation NMR
- Molecular Motion (Tumbling or Conformation
Change) --gt - Change in Neighbors Dipolar Field (even if rigid
internal structure relating the pair)--gt - Transitions/Relaxation if Tumbling is on
resonance with transition
U-(m0/4p)m1. m2-3(m1.R)(R. m2) (m0/2p)m1.
m23/2ltcos2qgt-1/2
20Transition Probability
- If transition is due to the field F from
neighboring dipole (fluctuating angular relation
between the dipoles described by unit vector R),
then the correlation function of interest is - Ensemble Averaged, Assumption of random motion
with a single correlation time
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23??c 3?mol.
24Saturation Recovery SQ vs DQ vs ZQ
- T1 SQ, DQ, ZQ relieve sat.
- NOE Perturbation of neighbor S Only ZQ and DQ
are effective
25Spin-Lattice Relaxation
- Note for 500 MHz, 13C-1H pair at 1.1 A,
correlation time of 1nsec - R1 4 s-1
26NOE Relaxation
- ?ij K (r-6) F(?c )
- Where K (?02/2?2)(1/10) (?H4h2/4?2)
- And F(?c ) ( -?c 6?c/(14?2?c2) )
-
- Note for two protons at 1A, with F(?c ) 1nsec
- 57.0 sec-1.
27NOE Molecular Weight, and Relaxation
- Spectral Density is provided at all frequencies
below the tumbling time - Medium sized or small protein tumbling time 5ns
(1ns/2.4 kDa) - DQ timescale is sub-nanosecond (inactive)
- ZQ is millisecond (active) negative NOE (peak
shrinks - For small molecules DQ more active positive NOE
- For peptides, equally active cancellation
condition no NOE
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30 31Typical Correlation Times and Relaxation Mobility
- Large protein DQ timescale is sub-nanosecond
(inactive), ZQ is millisecond (active) - If a region (loop, terminus) has independent
mobility it may exhibit cancellation condition.
This is strong evidence for a rapidly moving
segment (not necc. unstructured though)
32NOE Distance Interpretation
- Use a calibration peak (rigid proton pair)
- Assume Vk/r6 to estimate other distances
- Highly inaccurate
- Distances up to about 5A can be detected, several
tertiary contacts per residue generally obtained