Site-directed Spin Labeling (SDSL)and
Electron Paramagnetic Resonance (EPR)Spectroscopy
An Introduction
1
Johann P. Klare
Department of Physics, University of Osnabrück, 49069 Osnabrück, Germany
2
Outline
EPR Spectroscopy – A short introduction
What is a spin label?
Spin labeling of proteins: the „classical“ approach
EPR-Tools: What can we learn from spin labeled biomolecules
Spin-Spin Distance Determination
Spin Labeling Techniques
A general protocol for spin labeling using cysteine-specific reagents
3
Electron Paramagnetic Resonance (EPR)
or
Electron Spin Resonance (ESR)
EPR is the resonance spectroscopy of molecular systems with an unpaired electron.
What is it ?
4
Does my system have unpaired electrons?...
Organic Radicals in proteins
amino acid radicals (tyrosine...) protein bound cofactor radicals
(semiquinones, flavines)
cytochrome c oxidase
myoglobin
Metal centres in proteins /protein complexes Cu, Mn, Ni, Co, Mo, Fe hemes, FeS clusters
cytochrome bc1 complex
Short-lived radicals / Reactive Oxygen Species (ROS) Spin Traps / Spin Probes
O2-O2-O2-
++
5
Why Spin labelling?
(Most) proteins and nucleic acids don’t have unpaired electrons ! no EPR ?!
...but...
we can introduce the wanted unpaired electron into almost any system under investigation
and we can do this also (almost) wherever we want
Site-directed spin labeling (SDSL) Site-directed spin labeling (SDSL)
6
Does my system have unpaired electrons?...
Organic Radicals in proteins
amino acid radicals (tyrosine...) protein bound cofactor radicals
(semiquinones, flavines)
cytochrome c oxidase
myoglobin
Metal centres in proteins /protein complexes Cu, Mn, Ni, Co, Mo, Fe hemes, FeS clusters
cytochrome bc1 complex
Spin labels attached to proteins
or nucleic acids
Short-lived radicals / Reactive Oxygen Species (ROS) Spin Traps / Spin Probes
O2-O2-O2-
++
7
The Electron Spin
Elementary particles such as an electron (and also atomic nuclei !) are characterized by an intrinsic angular momentum: The Spin S!
→ they behave like spinning tops
Elementary particles are quantum particles – the rules of quantum mechanics apply !
The Spin can be in two states, which differ in the orientation of the angular momentum.
The Spin makes the electron behave like a tiny magnet !The Spin makes the electron behave like a tiny magnet !
mS = ½ & mS = - ½mS = ½ & mS = - ½
8
The Electron Spin in a Magnetic Field: The Concept of Magnetic Resonance
undisturbed electron in an external magnetic field B
Zeeman Effect or Electron-Zeeman Effect Zeeman Effect or Electron-Zeeman Effect
without a magnetic field, the two spin states of the electron are degenerate they have the same energy
if we place the electron in a magnetic field, the two spin states will have different energies (the energy levels are separated by DE).
9
The Resonance Condition
First: What does resonance mean ?
(Microwave) radiation is used for the transition of molecules from one state to the other:
lower state → higher state (absorption)higher state → lower state (stimulated emission)
Normally, we have more molecules (n0) in the (energetically) lower state (ground state) than in
the higher state (n1) (excited state) according to the Boltzmann distribution
Resonance results in net absorption of radiation. Resonance results in net absorption of radiation.
n1 = n0 ∙ exp(-DE/kT) k = Boltzmann constant
(1,381 · 10−23 J/K)
The Resonance condition for a two-level system in EPR is
hn = g b Bhn = g b B
Energy of the radiation
Energy difference between the twomolecular states produced by B.
Frequency n (or often angular frequency w = 2p∙n), for which the resonance condition is fulfilled:
Larmor FrequencyFrequency n (or often angular frequency w = 2p∙n), for which the resonance condition is fulfilled:
Larmor Frequency
10
We can explain our first EPR spectrum !
hn = g b Bhn = g b B
3280 3300 3320 3340 3360 3380
-40000
-20000
0
20000
40000
EP
R s
ign
al
Field / Gauss
DPPH
DPPH (Diphenylpikrylhydrazyl)A common standard for field calibration in EPR → g = 2.0036+/-0.0002
In most EPR machines the 1st
derivative of the absorptionspectrum is recorded !
(→ Field Modulation)
n 9.5 GHz (X band)
11
...most EPR spectra have more then one line...
another submolecular magnet comes into play:
the nucleus with its nuclear spin I Multiplicity:
Metal Isotope Spin Multiplicity
Mn 55 5/2 6
Fe54,56,57,58
1/2 (2%) 2
Co 59 7/2 8
Cu 63, 65 3/2 4
Mo92,94,95,96,97,98,100
5/2 6
Biological transition metal ions
Ligand Isotope Spin Multiplicity
H 1, 2 1/2, 1 (0.02%) 2, 3
C 12, 13 1/2 (1.1%) 2
N 14, 15 1, 1/2 3, 2
O 16,17,18 5/2 6
P 31 1/2 2
Cl 35,27 3/2 4
Ligand atoms
MI = 2I + 1MI = 2I + 1
Multiplicity = number of EPR lines
12
Types of Interactions
EPR spectra can reflect many different magnetic interactions, giving rise to (sometimes complicated) multi-line spectra.
...but (good news)...
We can describe and analyse most of the spectra just by considering
pairwise interactions between magnets of three types:
1. electron spins S2. nuclear spins I3. laboratory magnets B
We can describe and analyse most of the spectra just by considering
pairwise interactions between magnets of three types:
1. electron spins S2. nuclear spins I3. laboratory magnets B
...and (even better news)...
This results in five basic types of interactions, from which two are usuallyso weak, that we can ignore them !
13
Types of Interactions
electron spins Snuclear spins Ilaboratory magnets B
electron spins Snuclear spins Ilaboratory magnets B
Interaction Phenomenon Example
S x B Zeeman Interaction Basic EPR Pattern
S x I Hyperfine InteractionsMetal hyperfine (e.g. Cu (I=3/2))
“Ligand” hyperfine (1H (I=½), 14N (I=1))
S x SZero-Field Interactions
Dipolar Interactions
I x I Quadrupole Interaction Mn (I = 5/2)
I x BNuclear Zeeman
InteractionDouble Resonance Spectra (ENDOR)
and NMR !!
14
Interaction of the Electron Spin with Nuclear Spins: Hyperfine Interaction S x IS x I
The electron experiences not just one,but MI different “types” of nuclei (withdifferent local magnetic fields!).
Each “type” causes its own shift in the EPR resonance line
Hyperfine interaction for a Nitroxide radical (S = ½, I = 1)
A – Hyperfine constantA – Hyperfine constant
Multiplicity:
MI = 2I + 1MI = 2I + 1
Splitting into MI EPR lines ! Splitting into MI EPR lines !
15
Types of Interactions
electron spins Snuclear spins Ilaboratory magnets B
electron spins Snuclear spins Ilaboratory magnets B
Interaction Phenomenon Example
S x B Zeeman Interaction Basic EPR Pattern
S x I Hyperfine InteractionsMetal hyperfine (e.g. Cu (I=3/2))
“Ligand” hyperfine (1H (I=½), 14N (I=1))
S x SZero-Field Interactions
Dipolar Interactions
I x I Quadrupole Interaction Mn (I = 5/2)
I x BNuclear Zeeman
InteractionDouble Resonance Spectra (ENDOR)
and NMR !!
16
S x SS x SDipolar InteractionsDipolar Interactions
A not so simple equation (the Hamiltonian describing the dipole-dipole interaction)...
...with a simple message:
The dipolar interaction between two electrons is proportional to r -3,r being the distance between the two electrons.The dipolar interaction between two electrons is proportional to r -3,r being the distance between the two electrons.
Quantification of the dipolar interaction allows us to determine the distance between two paramagnetic centers!Quantification of the dipolar interaction allows us to determine the distance between two paramagnetic centers!
S1 and S2: spin operators for electrons 1 and 2.
^ ^
...what is dipolar interaction?
...how to quantify ? ...
17
S x SS x SDipolar InteractionsDipolar Interactions
...what is dipolar interaction ?
angular frequency w(at a fixed B field position)
hn = g b Bhn = g b B
w = 2p∙n
ħw = g b Bħw = g b B
resonance frequency of spin 1without dipolar interaction
18
...what is dipolar interaction ?
angular frequency w(at a fixed B field position)
dipolar interaction with parallel spin 2 B field at spin 1 is decreased lower resonance frequency
resonance frequency of spin 1with dipolar interaction withparallel aligned spin 2
S x SS x SDipolar InteractionsDipolar Interactions
hn = g b Bhn = g b B
w = 2p∙n
ħw = g b Bħw = g b B
19
...what is dipolar interaction ?
angular frequency w(at a fixed B field position)
resonance frequency of spin 1with dipolar interaction withantiparallel aligned spin 2
dipolar interaction with antiparallel spin 2 B field at spin 1 is increased higher resonance frequency
S x SS x SDipolar InteractionsDipolar Interactions
hn = g b Bhn = g b B
w = 2p∙n
ħw = g b Bħw = g b B
20
...what is dipolar interaction ?
angular frequency w(at a fixed B field position)
dipolar frequency wdddipolar frequency wdd
wdd (r) r-3wdd (r) r-3
S x SS x SDipolar InteractionsDipolar Interactions
hn = g b Bhn = g b B
w = 2p∙n
ħw = g b Bħw = g b B
21
Outline
EPR Spectroscopy – A short introduction
What is a spin label?
Spin labeling of proteins: the „classical“ approach
EPR-Tools: What can we learn from spin labeled biomolecules
Spin-Spin Distance Determination
Spin Labeling Techniques
• Proteins
• Nucleic Acids
A general protocol for spin labeling using cysteine-specific reagents
22
What is a spin label?
...a stable chemical compound which possesses an unpaired electron (i.e. it is a stable radical) and a specific reactive group to be bound to (bio)molecules....a stable chemical compound which possesses an unpaired electron (i.e. it is a stable radical) and a specific reactive group to be bound to (bio)molecules.
The vast majority of spin labels are nitroxides, where the unpaired electron is locatedat an –NO group, which is usually part of a heterocyclic ring.
A little bit of history:Spin labels were first synthesized in the laboratory of H. M. McConnell in 1965.The first spin labeling studies have been performed using thiol-specific functional groups to label natively occuringcysteines in proteins (e.g. in hemoglobin).Site-directed spin labeling (SDSL) was pioneered in the laboratory of Dr. W.L. Hubbell in the late 80’s/early 90’s.
Functional groups contained within the spin label allow them to be attached to the moleculeunder investigation and determine their specificity.
e.g.: Protein thiol groups specifically react with the functional groups methanethiosulfonate, maleimide, and iodoacetamide,
creating a covalent bond with cysteine.
23
Site-directed spin labeling of proteins: the „classical“ approach
24
1. Spin Label Mobility
2. Accessibilitytowards paramagneticquencher molecules(NiEDDA, CrOx, O2)
→ Discrimination betweenlipid bilayer, aqueous phaseand protein interior
5. Spin-Spin Distancedetermination(~ 10 – 70 Å)
4. Transient StructuralChanges
Information about Structure and Dynamics
SDSL-EPR-Tools: Overview
3. Polarityof the SL Microenvironment
25
Spin Label Mobility
The (RT) EPR spectral shape is sensitive to the reorientationalmotion of the nitroxide side chain (partial motional averaging of the anisotropic components of the g- and hyperfine tensors).
For spin-labeled sites exposed to the bulk water, the nitroxidemobility is slightyl restricted.
rotational correlation times in the ns range. small line widths of the center lines, DH0
small apparent hyperfine splittings.
Restricted mobility of the spin label side chain(interaction with neighboring side chains or backbone atoms)
line widths and the apparent hyperfine splittingsare increased
26
Spin Label Mobility
Klare, J.P., Steinhoff, H.-J., Photosynth. Res. 102, 377-390 (2009)
The correlation between the inverse linewidth DH0-1 and the inverse of the spectral
second moment H2-1 allows a general classification of the region where the spinlabel is located.
The spectral second moment H2 quantifiesthe breadth of the EPR spectrum.
27
Spin Label Mobility - Identification/analysis of multiple components
Arrhenius plot(logarithm of the rotational correlation times of the twocomponents vs. 1/T)
van’t Hoff plot(natural logarithm of theratio of the two spectralcomponents vs. 1/T)
Example: Analysis of a temperature and ionic strength dependent equilibrium between a compact and a dynamic form of a protein domain.
Doebber et al, J.Biol.Chem. .283, 28691-28701 (2008)
The cw EPR spectra show two components (1 and 2)with different rotational correlation times tc.The cw EPR spectra show two components (1 and 2)with different rotational correlation times tc.
28
0 1 2 3 4 5 6 7
O2
N2
Am
plit
ud
e ce
ntr
al li
ne
CrOx
lipid
0 1 2 3 4 5 6 7
O2
N2
Am
plit
ud
e ce
ntr
al li
ne
CrOx
water
0 1 2 3 4 5 6 7
O2
N2
Am
plit
ud
e ce
ntr
al li
ne
CrOx
2/1mWP
protein
Klare, J.P., Steinhoff, H.-J., Photosynth. Res. 102, 377-390 (2009)
P1/2 [Relaxing agent]- P1/2 [N2] [Relaxing agent]
[Relaxing agent]
P1/2
Accessibility for Paramagnetic Quencher Molecules
29
Polarity of the SL Microenvironment
Polarity and proticity of the spin label microenvironmentare reflected in
the hyperfine component Azz
the g tensor component gxx
A polar environment shifts
Azz to higher values gxx to lower values
polarity
Azz can be readily obtained from X band spectra.
To obtain gxx we need to goto W band (at least).
30
Assignment of secondary structures – Mobility, Accessibility, Polarity
Mobility Analysis
Polarity Analysis
Accessibility Analysis
324
320
310
300294
313
PutP
A Na+/prolinesymporter
31
Monitoring Transient Structural Changes
Klare, J.P., Steinhoff, H.-J., and Engelhard, M. (2004) FEBS Lett. 564 , 219
F
GTM2
Conformational changes in an archaebacterial photoreceptor/-transducer protein complex upon light excitation.
Position 159: change of the EPR signal due to transient mobilisation upon outward motion of helix FPosition 78 : change of the EPR signal due to increased dipolar interaction between the two spin labels
32
Spin-Spin Distance Determination
Low Temperature CW EPR (1-2 nm)
Double Electron Electron Resonance (DEER) (2-8 nm)
Simulation of EPR distance distributions
...or how to translate the EPR data into a model of your biomolecule
º molecular dynamics (MD) simulations
º the rotamer library approach (RLA)
33
Spin-Spin Distance Determination
Dipolar InteractionsDipolar Interactions
w
dipolar frequency wdddipolar frequency wdd
wdd (r) r-3wdd (r) r-3
broadening ofcw EPR spectrabroadening ofcw EPR spectra
34
Steinhoff et al. (1997) Biophys. J. 73, 3287-3298.
Low Temperature CW EPR:
35
Steinhoff et al. (1997) Biophys. J. 73, 3287-3298.
Low Temperature CW EPR:
36
Low Temperature CW EPR:
Steinhoff et al. (1997) Biophys. J. 73, 3287-3298.
37
Pulse Electron Double Resonance (PELDOR)or Double Electron-Electron Resonance (DEER)
dipolar frequency wdddipolar frequency wdd
wdd (r) r-3wdd (r) r-3
38
PELDOR/DEERPELDOR/DEER
G domain dimerization of the tRNA-modifying enzyme MnmE monitored with PELDOR.(Meyer et al., PLoS Biol. 7, e1000212 (2009))
39
Spin Labeling Techniques
Proteins
Spin labeling of cysteines Spin labeling by peptide synthesis Spin labeling using “click chemistry” Spin labeling using the nonsense suppressor methodology
ProteinsProteins
Nucleic Acids
Usage of spin labeled nucleotide analogs in oligonucleotide synthesis Postsynthetic modification of nucleotide analogs with reactive groups Postsynthetic modification at the sugar/phosphate backbone
Nucleic AcidsNucleic Acids
40
Spin Labeling of Cysteines
1. Methanethiosulfonate spin labels
MTSSL
MTSSL comprises a flexible linker minimizing disturbances of the
native fold of the protein !Size: comparable to that of a
tryptophane side chain.
MTSSL structure
MTSSL: (1-oxyl-2,2,5,5-tetramethylpyrroline-3-methyl) methanethiosulfonate
Formation of adisulfide bond:
→ sensitivity towardsreducing conditions !
MTS-4-oxyl spin label
Besides MTSSL, a variety of other different nitroxide radical compoundsare commercially available, which
- have a longer or shorter linker- are sterically more demanding- are pH sensitive- ....
41
Spin Labeling of Cysteines
2. Maleimide spin labelsFormation of aC-S bond:
→ no sensitivity towardsreducing conditions !
...but... sterically more demanding
(disturbance of protein structure!) can react also with primary amines
(N-term., Lysine, Arginine)
3. (Iodo)acetamide spin labels
Formation of aC-S bond:
→ no sensitivity towardsreducing conditions !
→ long, flexible linker
...but... can react also with secondary amines
(esp. Histidine)
42
Spin Labeling by (solid phase) peptide synthesis (SPPS)
Using the method of (solid phase)peptide synthesis, polypeptideswith arbitrary amino acids (incl.spin labeled amino acids !) can besynthesized.
Spin label building blocks for thestandard Boc- or Fmoc-basedpeptide synthesis have been syn-thesized or are commerciallyavailable.
The most popular spin label building block is the paramagnetic α-amino acid TOAC(4-amino-1-oxyl-2,2,6,6,-tetramethyl-piperidine-4-carboxylic acid).
TOAC exhibits only one degree of freedom: the ring conformation.
direct information about the orientation of secondarystructure elements !
Drawback of the method: Peptide synthesis is still limited to < 200 amino acids !Drawback of the method: Peptide synthesis is still limited to < 200 amino acids !
43
Spin Labeling by peptide synthesis - Expressed Protein Ligation (EPL)
Semisynthesis of proteins from recombinant and synthetic fragmentsSemisynthesis of proteins from recombinant and synthetic fragments
two polypeptide fragments:
peptide 1 (recombinant)peptide 2 (synthetic,
carrying the spin label)
formation of a native peptide bondbetween the two fragments by chemical ligation.
44
Spin Labeling using „click chemistry“
Highly selective formation of a carbon-heteroatom bond under mild conditions (→ stability of the nitroxide radical)and with high yield.
1,3-dipolar cycloaddition of organic azides with alkynes in the presence of Cu(I) (copper-catalyzed azide-alkyne 1,3-dipolar cycloaddition,CuAAC)
45Spin Labelling
Spin Labeling of nucleic acids
labeling of the nucleobase
labeling of the “backbone” sugar
46Spin Labelling
1. Usage of spin labeled nucleotide analogs in oligonucleotide synthesis
Chemically synthesized nucleotide analogs are used in standardoligonuleotide synthesis.Example: Spin-labeled thymidine analog, where a methyl group
is replaced by an acetylene-tethered nitroxide →
2. Postsynthetic modification of nucleotide analogs with reactive groups
Usage of nucleotide analogs chemically modified with reactive groups suitable forpost-synthetic modification with a spin labeling reagent.Example: 4-thiouridine (for RNA) derivatives, which can be modified with
thiol-specific reagent like MTSSL.
Spin Labeling of nucleic acids
47
Postsynthetic modification at the sugar/phosphate backbone
Alternatively, the spin label can be attached to the sugar moiety of specific nucleotides
Example: Postsynthetic derivatization of a 2’-amino group introduced into oligonucleotides with a isocyanatederivative of a TEMPO-like moiety.
Ward et al., ChemBioChem 8, 1957-1964 (2007)
48
A general protocol for spin labeling using cysteine-specific reagents
1. Spin labeling in solution
Incubate the purified protein for 1-2 h with a reducing agent (DTT, DTE) to reduce oxidized thiol groups.
Remove the reducing agent completely (!) by an appropriate method (washing in centrifugal concentrators, gel filtration, affinity chromatography (for proteins carrying an affinity tag), desalting columns, dialysis). Use a protective atmosphere (N2, Ar) to prevent re-oxidation.
Adjust the protein concentration be < 500 µM.
Incubate the protein with a 2-5fold excess (subject to optimization) of the spin label reagent.(Spin label compounds like MTSSL are usually quite hydrophobic. Stock solutions of 100 mM spin labelin e.g. DMSO have been proven to be convenient for most cases.)
The duration and the temperature at which incubation is performed depends on the actualsystem. Incubations over night at 4°C or 2-12h at RT usually lead to good labeling efficienciesfor well-accessible labeling sites. (Also this point is subject to optimization)
Remove unbound/unreacted spin label. The same procedure as for the removal of the reducingagent could/should be applied.
Check the labeling efficiency !
Check the functionality of the labeled protein protein/biomolecule !!!
49
A general protocol for spin labeling using cysteine-specific reagents
2. Spin labeling on affinity columns
Bind the protein to the affinity column. (Spin labelling could be the last step of your protein purification, just before you would elute it from the column)
Incubate the purified protein for 1-2 h with a reducing agent (DTT, DTE) to reduce oxidized thiol groups.
Wash out the reducing agent completely (!).
Incubate the protein with a 2-5fold excess (subject to optimization) of the spin label reagent.(Spin label compounds like MTSSL are usually quite hydrophobic. Stock solutions of 100 mM spin labelin e.g. DMSO have been proven to be convenient for most cases.)
The duration and the temperature at which incubation is performed depends on the actualsystem. Incubations over night at 4°C or 2-12h at RT usually lead to good labelling efficienciesfor well-accessible labelling sites. (Also this point is subject to optimization)
Wash out unbound/unreacted spin label.
Elute the protein from the column.
Check the labeling efficiency !
Check the functionality of the labeled protein protein/biomolecule !!!