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IR-spectroscopy Theory Applications to biomolecules and proteins
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IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Apr 02, 2018

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Page 1: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

IR-spectroscopy

TheoryApplications to

biomolecules and proteins

Page 2: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Infrared spectroscopy

• Transitions between vibrational levels in the ground state

Page 3: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Lower energies than VIS

Page 4: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Infrared spectroscopy• Transitions between vibrational levels in the

ground state• The intensity is related to the transition dipole

moment• Dichroism can be observed in oriented states• Polymers give new spectral features compared

to monomers due to coupling between adjacent transition dipole moments

Page 5: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

The intensity of a vibrational absorbtion band depends on the size of the transition dipole moment..

ba = <b || a >

How do wave functions look like for the ground state and the vibrationally excited state? NOTE: we must take both nuclei and electrons into account for vibrational transitions, since the nuclei are vibrating!

vv ’ (re , rn )

Page 6: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Born-Oppenheimer-approximation

We can divide the total wave function into

for the contribution of the elektrons

N for the contribution of the nuclei

(re : elektron coordinates, rn : coordinates of the nuclei) .

Then we can write the wave function as

State v State v ’

(re , rn ) =

(re , rn )

N (rn )

and the transition as

(re , rn )

Nv (rn ) (re , rn )

Nv’ (rn )

Page 7: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

What do the wave functions look like for the ground state and the excited vibrational state?

NOTE: we must take both nuclei and electrons into account for vibrational transitions!

Born-Oppenheimer-approximation: We can divide the total wave function into contributions from the electrons () and contributions from the nuclei (). r: elektron coordinates, R: nuclear coordinates). Then we can write the transition as

The intensity of a vibrational absorbtionsband depends on the size of the transition dipole moment..

ba = <b || a >

Page 8: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

But if the nuclei vibrate, it is possible to show by using taylor expansion ( where q = 0 is the equilibrium position of the nuclei) that the expectation value becomes:

If the nuclei are at rest the transition dipole moment only consists of , and becomes 0 since Nv, Nv’ are ortogonal

The alteration in dipole moment when the nuclei alter position

* Nv *

Nv’ d

*

d

Nv * Nv’ d

* Nv *

Nv’ d

* [ re q]q=0 d

Nv * q Nv’ d

If the dipole moment is altered during the vibration, IR absorbtion will occur!

Page 9: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Classical analogy:

= qR , /R = q

+q -qR The larger the charges, the larger the dipole moment – and the larger the absorbtion!

If the dipole moment of the molecule is altered during vibration, IR absorbtion will occur:

Page 10: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Biom

olecularIR absorbtion

band

Page 11: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

VWe can see alterations in molecular binding character.

Identification of synthesized substances (-OH, -COOH, -COH)

Characterisation of material (most absorb IR)

Covalent bonds: enzymatic transitions

Non-covalent bonds: hydrogen bonds

Isotope shifts (1H mot 2H)

Hydrophobic bonds / VdW interactions: membranes, lipids

Protein structures

Biomolecular interactions

Page 12: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

What does the sample cell look like?

ATR (attenuated total reflection): A film of protein or membrane is placed onto the IRS crystal

Measurements in KBr pellet is easiest

In solution: physiological, but you will have H2 O-absorbtion

Choose window with care! Must be transparent (BF,CaF, ZnSe, NaCl osv)

Cuvett length ~6 M

Page 13: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Effects of water

Page 14: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

IR FT-IRSweep

the wavelength

region using

one

wave

length

at a timeFourier

Transform -

technologies

A large number of experiments to cover entire wavelength range

Number of ’successful’ experiments are few

A cord of frequences

Each

experiment is successful!

• Low signal-to-noise

• Takes time – most ’experiments’ give no result

• we get results rapidly

• adding up several experiments gives high sensitivity

Page 15: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

First experimental confirmation of Watson-Crick base pairing came from IR spectroscopy

A+U

AU

G+C

GC

Page 16: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

1:1 – base-to-base binding: evidence from IR titrations

Page 17: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Linear polarized light is widely applied in IR, since we can orient our samples onto the sample cell:

AII and A

can be related to molecular orientation.

Page 18: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Linear dichroism in oriented DNA molecules

Which curve shows T

and which shows

TII to the helix axis?

Page 19: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Linear dichroism in oriented DNA molecules

Vibration in the base plane results in larger absorbance/reduced transmission for light polarized parallel to the bases (orthogonal to the helix axis) since it is then parallel with the transition dipole moment.

From the difference between T II and T

the angle between the base plane and the helix axis can be calculated.

T

:

T II :

Page 20: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower
Page 21: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Difference spectra for two Ca2+-release reactions from phosphorylated (thin line) and non-phosphorylated ATP-ase (thick line)

Barth et al., JBC 1997

Covalent bonds: intermediates and products in enzymatic reactions

Page 22: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Time-resolved spectra (0.3-0.4 ms difference) from different photo-induced intermediates of bacteriorhodopsin

Page 23: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Can we observe protein structure?

Tsuboi, J. Poly. Sci., 1962

Poly-g-benzyl-L-glutaminsyra Heldragen linje: ljus polariserat parallellt med fiberriktningen

Streckad linje: polariserat ljus ortogonalt mot fiberriktningen

Page 24: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

How sensitive is IR to secondary structure?

-helix

Random coil

-sheet

Page 25: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Interactions between transition dipoles renders transitions to be allowed or forbidden

Antiparallel -sheet -helix

Miyazawa, J Chem Phys, 1960

D10 > D30 > D20

Page 26: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower
Page 27: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

How is secondary structure evaluated?

-Evaluation using the second derivative

-Fourier self-deconvolution (spectral deconvolution)

Page 28: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Example of evaluation process

-sheet

irregularDifferent kinds of -sheet

Steg 1 Steg 2

Page 29: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Membrane proteins we can study both the protein …

Bundle Monomer

Dynamic / 310 helix Dynamic/310 -helix

-helix-sheet/turn

Random coil

Page 30: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

… and its effects on the lipid

ATR dichroism spectra of multibilayers without…

… and with protein: an organization!

Sal-Man et al., Biochemistry 2002, Preassembly of membrane active peptides is an important factor in their selectivity toward target cells.

Page 31: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Denaturation

Nativt tendamistat: denaturation midpoint (Tm) at 82 ºC

Mutated tendamistat: Lower Tm, aggregation at higher temperatures

Page 32: IR-spectroscopy - IFM · IR-spectroscopy Theory Applications to biomolecules and proteins. Infrared spectroscopy • Transitions between vibrational levels in the ground state. Lower

Which situation results in significant changes in difference spectra?