Infrared Spectroscopy & Circular Dichroism Haydyn Mertens PhD - - PowerPoint PPT Presentation

infrared spectroscopy circular dichroism
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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


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Infrared Spectroscopy

&

Circular Dichroism

Haydyn Mertens PhD

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Infrared Spectroscopy

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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

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Stretching of bonds (eg. water)

Vibrational modes

Symmetric Asymmetric Bending

3 fundamental vibration modes

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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)

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Wavenumber number of wavelengths (l) per distance

Units for IR spectroscopy

v = 1/l (cm-1)

proportional to frequency proportional to photon energy

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Infrared (IR) Absorption: Proteins

Barth & Zscherp, Quart. Rev. Biophys. 2002, 35(4), 369-430.

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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

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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

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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

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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

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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

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Limited information available. Lack of spatial information. Spectral congestion

1D FTIR: Proteins

Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441

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fs pulsed spectroscopy Frequency domain (pump-probe) Time domain (echo)

2D-FTIR

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fs pulsed spectroscopy Coupled systems See coherences

2D-FTIR

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Small molecule example: acetyl-acenato-rhodium dicarbonyl (RDC)

2D-FTIR

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2D-FTIR: Proteins

Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441

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Characteristic "shapes"

Spectral patterns for secondary structure

Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441

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Characteristic "shapes"

Ganim et al., Acc. Chem. Res., 2008, 41 (3), pp 432–441

Z-shape Figure-8

Diagonally elongated

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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)

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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

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Amide I labeling 13C-16O/18O

Specific labeling Shifts absorption band (red-shift) Reduces problem of spectral crowding

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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

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Measure vibrational modes Identify secondary structure Monitor protein unfolding Investigate conformational change

Summary FTIR

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Circular Dichroism

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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

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Differential Absorption

eL - eR ∆e +

  • e

Adapted from: Johnson, Ann. Rev. Biophys. Chem. 1988. 17: 145-66.

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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

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General scheme of electronic transitions

Amide Chromophores

n n 2pz

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Amide Chromophores

Transition dipoles n

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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

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helix, sheet and "other"

Characteristic CD Spectra

Myoglobin Concanavalin A beta-lactoglobulin Type VI collagen

∆฀ +

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The alpha-helix

n ---> pi* pi1 ---> pi* pi1 ---> pi*

∆฀ +

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The beta-sheet

n ---> pi* pi1 ---> pi* pi1 ---> pi*

∆฀ +

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"Other" (Random coil)

pi1 ---> pi*

pi1 ---> pi*

∆฀ +

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Differential ABS left and right polarised light

Circular Dichroism

www.jascoinc.com

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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

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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

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Contin-LL Selcon 3 CDSSTR VARSLC K2d Dichroweb server http://dichroweb.cryst.bbk.ac.uk

Programs