Protein-Nucleic Acid Dynamics Ashok Kolaskar Vice Chancellor University of Pune Pune India.
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Transcript of Protein-Nucleic Acid Dynamics Ashok Kolaskar Vice Chancellor University of Pune Pune India.
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Protein-Nucleic Acid Dynamics
Ashok Kolaskar
Vice Chancellor
University of Pune
Pune
India
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Molecular Dynamics: Introduction
Biomolecules are
polymers of basic building blocks
Proteins Amino Acids
Nucleic acids Nucleotides
Carbohydrates Sugars
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Molecular Dynamics: Introduction
• At physiological conditions, the biomolecules undergo several movements and changes
• The time-scales of the motions are diverse, ranging from few femtoseconds to few seconds
• These motions are crucial for the function of the biomolecules
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Molecular Dynamics: Introduction
Newton’s second law of motion
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We need to know
The motion of the
atoms in a molecule, x(t) and therefore,
the potential energy, V(x)
Molecular Dynamics: Introduction
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Molecular Dynamics: IntroductionHow do we describe the potential energy V(x) for amolecule?Potential Energy includes terms for
Bond stretching
Angle Bending
Torsional rotation
Improper dihedrals
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Molecular Dynamics: Introduction
Potential energy includes terms for (contd.)
Electrostatic
Interactions
van der Waals
Interactions
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Molecular Dynamics: Introduction
Equation for covalent terms in P.E.
)](cos1[)(
)()(
02
0
20
20
nAk
kllkRV
torsions
n
impropers
anglesbonds
lbonded
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Molecular Dynamics: Introduction
Equation for non-bonded terms in P.E.
ijr
ji
ij
ij
ij
ij
ji
nonbonded r
r
r
r
rijRV
0
6min
12min
4])(2)[(()(
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Molecular Dynamics: Introduction
• Each of these interactions exerts a force onto a given atom of the molecule
• The total resulting force on each atom is calculated using the PE function
Knowing the force on an atom, its movement due to the force is then calculated:
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Molecular Dynamics: Introduction
To do this, we should knowat given time t,
• initial position of the atom
x1
• its velocity
v1 = dx1/dt• and the acceleration
a1 = d2x1/dt2 = m-1F(x1)
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Molecular Dynamics: Introduction
The position x2 , of the atom after time interval t would be,
and the velocity v2 would be,
tvxx 112
tdx
dVmvtxFmvtavv x
1
111
11112 )(
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How a molecule changes during MD
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Molecular Dynamics: Introduction
In general, given the values x1, v1 and the potential energy V(x), the molecular trajectory x(t) can be calculated, using,
tdx
xdVmvv
tvxx
ixii
iii
1
)(11
11
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• Generalizing these ideas, the trajectories for all the atoms of a molecule can be calculated.
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The Necessary Ingredients
• Description of the structure: atoms and connectivity
• Initial structure: geometry of the system• Potential Energy Function: force field
• AMBER• CVFF• CFF95• Universal
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Protein-specific Applications of MD
• Calculation of thermodynamic propertiessuch as internal energy, free energy
• Studying the protein folding / unfolding process
• Studying conformational properties and transitions due to environmental conditions
• Studying conformational distributions in molecular system.
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MotionSpatial extent
(nm)
Log10 of characteristic
time (s)
Relative vibration of bonded atoms
0.2 to 0.5 -14 to –13
Elastic vibration of globular region
1 to 2 -12 to –11
Rotation of side chains at surface
0.5 to 1 -11 to –10
Torsional libration of buried groups
0.5 to 1 -14 to –13
An overview of various motions in proteins (1)
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MotionSpatial
Extent (nm)
Log10 of characteristic
time (s)
Relative motion of different globular regions
(hinge bending) 1 to 2 -11 to –7
Rotation of medium-sized side chains in interior
0.5 -4 to 0
Allosteric transitions 0.5 to 4 -5 to 0
Local denaturation 0.5 to 1 -5 to 1
Protein folding ??? -5 to 2
An overview of various motions in proteins (2)
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A typical MD simulation protocol
• Initial random structure generation
• Initial energy minimization
• Equilibration
• Dynamics run – with capture of conformations at regular intervals
• Energy minimization of each captured conformation
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Essential Parameters for MD (to be set by user)
• Temperature
• Pressure
• Time step
• Dielectric constant
• Force field
• Durations of equilibration and MD run
• pH effect (addition of ions)
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WHAT IS AMBER?AMBER (Assisted Model Building with Energy Refinement).
Allows users to carry out molecular dynamics simulations
Updated forcefield for proteins and nucleic acids
Parallelized dynamics codes
Ewald sum periodicity
New graphical and text-based tools for building molecules
Powerful tools for NMR spectral simulations
New dynamics and free energy program
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WHY AMBER?Most widely used program: approximately 5000 users world over.
Over 1000 research papers have been published using AMBER.
Program available at a nominal price for academic users.
Complete source code available with the package.
Available for most machine configurations.
Developed by Prof.Peter Kollman at the University of California San Francisco: An authority in the area of molecular simulations.
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BASIC INFORMATION FLOW IN AMBER
prep link edit parm
mdanal
nmode
Sander,
Gibbs,
spasms
anal
Nmanal,
lmanal
carnal
seq pdb forcefield
constraints
database
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CASE STUDY• Type II restriction endonucleases recognize DNA sequences of
4 to 8 base pairs in length and require Mg2+ to hydrolyse DNA.• The recognition of DNA sequences by endonucleases is still
an open question.• PvuII endonuclease, recognizes the sequence 5’-CAGCTG-3’
and cleaves between the central G and C bases in both strands.• Though crystal structure of the PvuII-DNA complex have
been reported, very little is known about the steps involved in the recognition of the cleavage site by the PvuII enzyme.
• Molecular dynamics (MD) simulation is a powerful computational approach to study the macromolecular structure and motions.
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CASE STUDY: METHODS (MD Simulations)• Simulations were carried out on the sequence
– 5’-TGACCAGCTGGTC-3’– Rectangular box (60 X 48 X 54 Å3) containing 24 Na+, using PBC– SHAKE algorithm– Integration time step of 1 fs– 283 K with Berendsen coupling– Particle Mesh Ewald (PME) method– 9.0 Å cutoff was applied to the Lennard-Jones interaction term.
• Equilibration was performed by slowly raising the temperature from 100 to 283 K. Production run was initiated for 1.288 ns and the structures were saved at intervals of one picosecond.
• The trajectory files were imaged using the RDPARM program and viewed and analysed using the MOIL-VIEW and CURVES packages respectively.
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STARTING DNA MODEL
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DNA MODEL WITH IONS
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DNA in a box of water
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SNAPSHOTS
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SNAPSHOTS
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SHORTENING
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AVERAGE ROLL
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AVERAGE TWIST
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RESULTSParticle Mesh Ewald simulations of PvuII substrate• The simulations carried out using PME method, points out that
the initial straight B-helix conformation bends significantly as the simulation progresses. The DNA molecule bends maximally by 18% and 22% at 616 ps and 1243 ps respectively. The base pair rise (h) between G7:C7’ and C8:G6’ observed in this simulation, shows large fluctuations around the normal value.
• The average roll value is seen to increase with simulation time and this indicates bending of the DNA molecule.
• The offset values, for each base pair showed that the maximum bending of the DNA molecule occurs at G7 and C8 bases.
• When viewed from the top, the snapshots of DNA structures captured at 50 ps interval show that the DNA structures move from a B-DNA structure to a close to an A-DNA.
• The average helical twist at the beginning of the simulation is an ideal B-DNA, and is about 31 upto 500 ps and beyond 500 ps, the twist is below that of an ideal A-DNA (28). This, along with phase indicates that the molecule is neither in an A-DNA nor a B-DNA form.
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DOCKING
• The MD frames bearing closest similarity to the conformation of the DNA in the PvuII-DNA crystal structure, were selected for docking, using the Affinity module in the MSI package.
• The molecules were subjected to MC minimization with a maximum translational move of 8 Å and a maximum rotational move of 360 Å. An energy tolerance parameter of 1000 was used.
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DOCKING RESULTS
• In order to understand the phenomena of the recognition and cleavage of the DNA substrate by the PvuII enzyme, the conformation of the PvuII enzyme as obtained from the complex crystal structure was docked to various frames of the DNA from the MD trajectory.
• The structure at the 1230 ps gave good stable energy of –1898 Kcal/mol after optimization due to stabilization arising from hydrogen bonds and nonbonded contacts between the amino acid side chains and the bases in the DNA. The structure at 1230 ps also showed a very high shortening of 22.31 % indicating that the molecule is highly curved.
• This suggests that the PvuII enzyme recognizes the bent conformation of the substrate DNA and binds to it.
• The shortening of the docked DNA was seen to be about 20.71 % as compared to 3.73 % for that of the DNA in the complex crystal structure, indicating that the enzyme prefers the bent DNA structure.
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DOCKING
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DOCKING
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CONCLUSION
• Our studies reported here for nanosecond MD simulations point out that the 13-mer DNA substrate for PvuII bends considerably.
• Docking studies showed that the PvuII enzyme recognizes the bent DNA conformation.
• The local distortions in the helical conformation at the base pair level may be playing an important role during the cleavage of the phosphodiester bond