apm 530 - lecture 2 - arizona state university€¦ · jay taylor (asu) apm 530 - lecture 2 fall...
TRANSCRIPT
Molecular Structure Background
Valence
Each element tends to form a fixed number of bonds that depends on thenumber of electrons in its outer shell:
Carbon and phosphorus havevalence 4
Nitrogen has valence 3
Oxygen and sulphur havevalence 2
Hydrogen has valence 1
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 1 / 20
Molecular Structure Background
Notation
Carbon atoms are oftenshown as vertices.
Hydrogen atoms boundto C are often implicit.
Nitrogen, Oxygen,Phosphorus, Sulphur atomsare explicit.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 2 / 20
Molecular Structure Background
Molecules can rotate about single bonds.
e− density is approximatelyradially symmetric about thebond.
Steric hindrance of attachedatoms can restrict themotion.
Timescale of rotation is∼ 10−11 sec.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 3 / 20
Molecular Structure Background
Double bonded compounds are planar.
No rotation about thedouble bond.
Two stereoisomers: cis(same side) and trans(opposite sides).
The trans isomer is usuallymore stable.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 4 / 20
Molecular Structure Background
Molecular structure can be represented using Cartesian or InternalCoordinates
Cartesian coordinates are used in most computations.
Potential energies are often expressed in terms of internal coordinates.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 5 / 20
Molecular Structure Background
Dihedral Angles
τijkl = cos−1(~nijk · ~njkl)
~nijk =~ij × ~jk
|~ij × ~jk|
The dihedral angle between linked atoms i − j − k − l is thecounterclockwise angle between the bond vectors ~kl and ~ij whenrotated about ~jk.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 6 / 20
Molecular Structure Background
Steric Interference
Repulsive forces between atoms can favor certain dihedral angles.
Staggered conformations are usually much more stable than eclipsedconformations.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 7 / 20
Molecular Structure Nucleic Acids
Backbone torsion angles
Backbone torsion angles controlDNA/RNA bending.
The angles α, · · · , ζ are measuredalong the sequence
P → O5′ → C5′ → C4′ → C3′
→ O3′ → P.
β and δ are usually in the transstate.
α, γ and ζ are more flexible.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 8 / 20
Molecular Structure Nucleic Acids
Ring Puckering
The pentose sugar is usuallynon-planar.
Twist conformations have threecoplanar atoms.
Envelope conformations havefour.
Atoms displaced to the sameside as C5’ are endo; those onthe other side are exo.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 9 / 20
Molecular Structure Nucleic Acids
The Pseudorotation Cycle
The endocyclic torsion anglesτ0, · · · , τ4 are defined clockwisefrom the 04’-C1’ bond.
These approximately obey theformula:
τj = ν cos
(P +
4π
5(j − 2)
),
where P is the phase and ν isthe amplitude.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 10 / 20
Molecular Structure Nucleic Acids
Glycosyl Rotation
Base flipping occurs through rotation from a syn to an anti conformation.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 11 / 20
Molecular Structure Nucleic Acids
Geometry of Helices
Helix sense (handedness)
Pitch Ph is the distance along thehelix axis for one turn.
Axial rise h is the vertical distancebetween adjacent base pairs.
nb is the number of base pairs per turn.
Unit twist is the rotation about thehelix axis between adjacent base pairs:Ω = 360/nb.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 12 / 20
Molecular Structure Nucleic Acids
Nucleic acid helices have a major and a minor groove.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 13 / 20
Molecular Structure Nucleic Acids
Base pair parameters
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 14 / 20
Molecular Structure Experimental techniques
X-ray crystallography
X-ray wavelengths 0.1− 10 A.
Molecular structure can beinferred from X-ray diffractionpatterns produced by crystals.
The amplitude of the scatteredwave is proportional to the FTof the density of nuclei p(~r):∫
d~r p(~r)e−i~q·~r ,
where ~q = ~kout − ~kin.
One limitation is that the molecules must usually be crystallized.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 15 / 20
Molecular Structure Experimental techniques
Nuclear Magnetic Resonance (NMR)
Structures of molecules insolution can be inferred usingmultidimensional NMR.
Nuclei exposed to EM pulsesradiate the energy at frequenciesthat depend on both bondedand non-bonded nuclei.
Information is available for H,C-13 and N-15.
NMR provides structural information about molecules in solution, but islimited to molecules with sizes < 100 kDa.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 16 / 20
Molecular Structure Helical structures
DNA helices can have different conformations.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 17 / 20
Molecular Structure Helical structures
Average properties of A-, B- and Z-DNA
Property A-DNA B-DNA Z-DNA
Handedness right right left
bps/turn 11 10-10.5 12
Rise/bp 2.6 A 3.4 A 3.8 A
Diameter 26 A 20 A 18 A
Pitch 28 A 34 A 45 A
bp inclination 20 0 −7
Sugar pucker C3’-endo C2’-endo C2’/C3’-endo
Glycosyl rotation anti anti anti (C)/syn (G)
Major groove narrow & deep wide & deep convex
Minor groove wide & shallow narrow & deep narrow & deep
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 18 / 20
Molecular Structure Helical structures
Occurrence of A-, B- and Z-DNA
B-DNA is the canonical form of DNA under physiological conditions.
A-DNA occurs at low humidity (e.g., in some crystals) and in someDNA-RNA hybrids and regions of dsRNA.
Z-DNA may occur transiently in negatively-supercoiled DNA and inpoly(dGC)2 sequences.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 19 / 20
Molecular Structure Helical structures
References
Krebs, J. E., Goldstein, E. S. and Kilpatrick, S. T. (2011) Lewin’sGenes X. Jones and Bartlett.
Schlick, T. (2006) Molecular Modeling and Simulation. Springer.
Jay Taylor (ASU) APM 530 - Lecture 2 Fall 2010 20 / 20