Infrared Spectroscopy & Circular Dichroism Haydyn Mertens PhD - - PowerPoint PPT Presentation
Infrared Spectroscopy & Circular Dichroism Haydyn Mertens PhD - - PowerPoint PPT Presentation
Infrared Spectroscopy & Circular Dichroism Haydyn Mertens PhD Infrared Spectroscopy Infrared Spectroscopy Electromagnetic spectrum: VIS med long-wave IR Short Gamma X-Ray UV IR microwaves radiowaves nm um mm m km Wavelength
Infrared Spectroscopy
Electromagnetic spectrum:
Infrared Spectroscopy
Functional groups absorb IR radiation Induced vibrational excitation
Wavelength 10-9 10-6 10-3 1 10 102 m nm um mm m km Gamma X-Ray UV IR microwaves
Short
radiowaves VIS med long-wave IR
Stretching of bonds (eg. water)
Vibrational modes
Symmetric Asymmetric Bending
3 fundamental vibration modes
Harmonic oscillator simple example
- eg. diatomic molecule
Vibrational modes
Vibrational frequency: v ∝ k*mr
eg. C=O, C=N (1500 - 1900 cm-1) C-H, N-H, O-H (2700 - 3800 cm-1)
Wavenumber number of wavelengths (l) per distance
Units for IR spectroscopy
v = 1/l (cm-1)
proportional to frequency proportional to photon energy
Infrared (IR) Absorption: Proteins
Barth & Zscherp, Quart. Rev. Biophys. 2002, 35(4), 369-430.
Traditional IR spectroscopy "dispersive" Monochromatic beam Measure absorbance Scan across different wavelengths FTIR Broadband used Excite multiple states/modes Adjust broadband and repeat Deconvolute spectrum
Infrared (IR) spectroscopy
Key component is the interferometer
FTIR spectroscopy
Detected signal: Intensity as function of mirror position (cm) FT to obtain IR spectrum (cm-1)
http://www.chem.agilent.com
Sensitive to secondary structure:
1D FTIR: Proteins
Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441
Amide I and Amide II modes
Sensitive to secondary structure:
1D FTIR: Proteins
Adapted from: Barth & Zscherp, Quart. Rev. Biophys., 2002, 35, pp 369-430
Amide I and Amide II modes
Sensitive to secondary structure:
1D FTIR: Proteins
Adapted from: Barth & Zscherp, Quart. Rev. Biophys., 2002, 35, pp 369-430
Amide I and Amide II modes
Limited information available. Lack of spatial information. Spectral congestion
1D FTIR: Proteins
Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441
fs pulsed spectroscopy Frequency domain (pump-probe) Time domain (echo)
2D-FTIR
fs pulsed spectroscopy Coupled systems See coherences
2D-FTIR
Small molecule example: acetyl-acenato-rhodium dicarbonyl (RDC)
2D-FTIR
2D-FTIR: Proteins
Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441
Characteristic "shapes"
Spectral patterns for secondary structure
Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441
Characteristic "shapes"
Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441
Z-shape Figure-8
Diagonally elongated
Access to fast time-scale:
10-13 s 104 s 10-11 s 10-6 s 10-3 s 10-9 s
Short-range fluctuations
(side-chains, torsion-angles, hydrogen bonds)
Secondary structure formation Domain folding (tertiary contacts) Folding/Binding (aggregation)
Thermal denaturation of Ubiquitin
(Chung et al., PNAS. 2007, 104, 14237-14242.)
Example: Protein Unfolding
2D FTIR from MD simulation Experiment
Folded Unfolded Difference
Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441
Amide I labeling 13C-16O/18O
Specific labeling Shifts absorption band (red-shift) Reduces problem of spectral crowding
M2 (influenza A), H+ gated ion channel Transmembrane helix conformation
13C=18O labeled residues as probes
Example: Membrane Protein
Manor et al., Structure. 2009, 17, pp 247-254.
Linewidth 13C=18O increases with solvent contact
Measure vibrational modes Identify secondary structure Monitor protein unfolding Investigate conformational change
Summary FTIR
Circular Dichroism
Absorbance spectroscopy of electronic transitions: A = e*c*l
e = extinction coefficient (depends on wavelength, l) c = concentration l = path length
CD is difference between e for left and right circularly polarized light
AL(l) - AR(l) = ∆A(l) = [eL(l) - eR(l)]*l*c
Circular Dichroism
Differential Absorption
eL - eR ∆e +
- e
Adapted from: Johnson, Ann. Rev. Biophys. Chem. 1988. 17: 145-66.
Protein backbone amides Electronic absorption (UV) Sensitive to orientation of transition dipoles amide n ---> pi* (210 nm) pi1 ---> pi* (190 nm) Sensitive to backbone dihedral angles thus secondary structure
Amide Chromophores
General scheme of electronic transitions
Amide Chromophores
n n 2pz
Amide Chromophores
Transition dipoles n
Absorption is modulated by Interactions between transitions:
pi1 ---> pi* coupling between peptide groups Mixing n ---> pi* and pi1 ---> pi* within a peptide group Mixing n ---> pi* and pi1 ---> pi* between peptide groups
Influenced by geometry of peptide backbones --> Secondary structure!!!
Secondary Structure
helix, sheet and "other"
Characteristic CD Spectra
Myoglobin Concanavalin A beta-lactoglobulin Type VI collagen
∆ +
The alpha-helix
n ---> pi* pi1 ---> pi* pi1 ---> pi*
∆ +
The beta-sheet
n ---> pi* pi1 ---> pi* pi1 ---> pi*
∆ +
"Other" (Random coil)
pi1 ---> pi*
pi1 ---> pi*
∆ +
Differential ABS left and right polarised light
Circular Dichroism
www.jascoinc.com
Using database of known structures Calculate amount of helix/sheet/other Secondary structure content Fold recognition More data (ie. VUV region) increases the information content
Information content
Secondary structure content Voltage-gated sodium channel Minimal functional tetramer designed
Example:
McCusker et al., J. Biol. Chem. 2011, March 15 (epub)
CD sprectrum (50 % helix) Melting curve (222 nm)
30% helix 19% helix