Download Protein Structure (in a nutshell)

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Endomembrane system wikipedia , lookup

Protein (nutrient) wikipedia , lookup

Proteasome wikipedia , lookup

Ubiquitin wikipedia , lookup

LSm wikipedia , lookup

Signal transduction wikipedia , lookup

Magnesium transporter wikipedia , lookup

G protein–coupled receptor wikipedia , lookup

Protein phosphorylation wikipedia , lookup

SR protein wikipedia , lookup

Ribosome wikipedia , lookup

JADE1 wikipedia , lookup

Protein moonlighting wikipedia , lookup

Protein wikipedia , lookup

List of types of proteins wikipedia , lookup

Homology modeling wikipedia , lookup

Circular dichroism wikipedia , lookup

Protein domain wikipedia , lookup

Protein folding wikipedia , lookup

Protein–protein interaction wikipedia , lookup

Nuclear magnetic resonance spectroscopy of proteins wikipedia , lookup

Intrinsically disordered proteins wikipedia , lookup

Protein structure prediction wikipedia , lookup

Proteolysis wikipedia , lookup

Transcript
Protein Structure
(in a nutshell)
Guy Ziv
December 26th, 2006
Myoglobin (1958)
Proteins




From the Greek “proteios” meaning
“of first importance”
The basic building blocks of almost all life
Constitutes the majority of the cell, and perform nearly all
enzymatic activities
Composed of 20 naturally occurring amino-acids
varying moiety
called “side chain”
Protein Synthesis In-vivo
1.
2.
3.
Transcription:
DNA  messenger RNA (mRNA)
Translation:
mRNA  Linear chain of a.a.
(Ribosome)
Folding:
Linear chain  Structure
Peptide bond
Protein chains have direction N-terminal → C-terminal
X-Rays crystallography –
the tool of structural biology



Why X-ray?
Wavelength of visible light: ~500 nm
Bond lengths in proteins: ~0.15 nm
Typical X-ray wavelength: ~0.15 nm
X-ray are (weakly) scattered by electrons
Diffraction from a single molecule is weak
so use a crystal:
–
–
Multiple copies of the molecule increases diffraction
Crystalline structure imposes constraints on diffraction
pattern
Diffraction occurs at particular angles

Diffraction
spots are the
result of
constructive
interference
from multiple
scatterers
satisfying
Bragg’s Law:
λ = 2 d sinθ
q
q
Bragg planes intersect the unit cell in
particular “indices”
0,0
k
h
h=1, k=1
h=4, k=-2
Each Spot Represents a Unique Set of
Bragg Planes
Points in k-space
(Fourier Space)
h=2, k=1, l=3
h=10, k=3, l=8
detector
λ = 2 d sinθ
q1
q2
q3
Modern X-Ray Crystallography
Early 1950’s
Need good crystals for better resolution,
which is difficult in proteins (need right conditions)
and sometimes nearly impossible
(e.g. membranal proteins)
High resolution details are faint – requires
good experimental apparatus
Recorded intensity give only the magnitude
but not the phase of the complex “form factor”
Error in density map lead to un-realistic
atom assignment, requiring iterative refinement
process
Historical perspective to
Pauling and Corey paper series



X-ray crystallography, invented in the beginning
of the 20’th century, has been used to solve
structures of some amino-acids, synthetic
polymers (poly-glu) and small organic molecules
Some fibrous materials such as wool and
α-keratin are sufficiently crystalline to give
diffraction patterns
Evidence suggested that these proteins’
structure involve mainly translation and rotation
Pauling and Corey
Robert Corey (1897-1971)
Linus Pauling (1901-1994)
Pauling and Corey papers series –
PNAS April 1951
1.
2.
3.
4.
5.
6.
7.
8.
Pauling, L., Corey, R.B. and Branson H. R. The Structure of Proteins:
Two Hydrogen-Bonded Helical Configurations of the Polypeptide
Chain. PNAS, 37, 205-211, (1951).
Pauling, L. & Corey, R. B. Atomic Coordinates and Structure Factors
for Two Helical Configurations of Polypeptide Chains. PNAS, 37,
235-240, (1951).
Pauling, L. & Corey, R. B. The Structure of Synthetic Polypeptides.
PNAS, 37, 241-250, (1951).
Pauling, L. & Corey, R. B. The Pleated Sheet, A New Layer
Configuration of Polypeptide Chains. PNAS, 37, 251-256, (1951).
Pauling, L. & Corey, R. B. The Structure of Feather Rachis Keratin.
PNAS, 37, 256-261, (1951).
Pauling, L. & Corey, R. B. The Structure of Hair, Muscle, and Related
Proteins. PNAS, 37, 261-271, (1951).
Pauling, L. & Corey, R. B. The Structure of Fibrous Proteins of the
Collagen-Gelatin Group. PNAS, 37, 272-281, (1951).
Pauling, L. & Corey, R. B. The Polypeptide-Chain Configuration in
Hemoglobin and Other Globular Proteins. PNAS, 37, 282-285, (1951).
Pauling and Corey papers series –
PNAS April 1951
1.
2.
3.
4.
5.
6.
7.
8.
Pauling, L., Corey, R.B. and Branson H. R. The Structure of Proteins:
Two Hydrogen-Bonded Helical Configurations of the Polypeptide
Chain. PNAS, 37, 205-211, (1951).
Pauling, L. & Corey, R. B. Atomic Coordinates and Structure Factors
for Two Helical Configurations of Polypeptide Chains. PNAS, 37,
235-240, (1951).
Pauling, L. & Corey, R. B. The Structure of Synthetic Polypeptides.
PNAS, 37, 241-250, (1951).
Pauling, L. & Corey, R. B. The Pleated Sheet, A New Layer
Configuration of Polypeptide Chains. PNAS, 37, 251-256, (1951).
Pauling, L. & Corey, R. B. The Structure of Feather Rachis Keratin.
PNAS, 37, 256-261, (1951).
Pauling, L. & Corey, R. B. The Structure of Hair, Muscle, and Related
Proteins. PNAS, 37, 261-271, (1951).
Pauling, L. & Corey, R. B. The Structure of Fibrous Proteins of the
Collagen-Gelatin Group. PNAS, 37, 272-281, (1951).
Pauling, L. & Corey, R. B. The Polypeptide-Chain Configuration in
Hemoglobin and Other Globular Proteins. PNAS, 37, 282-285, (1951).
Linus Carl Pauling
The Nobel Prize in Chemistry 1954
"for his research into the nature
of the chemical bond and its
application to the elucidation
of the structure of complex
substances"
Determinants of helical structure
superposition
Resonant partial double bond character of
peptide bond induces planar arrangement of
atoms
Distances and angles
Between atoms
All hydrogen bonds should be satisfied,
i.e. distance N-O of about 2.7Å and angle
between C = O and H – N less then ~30°
Building a model –
similar to building with LEGO blocks



Start assembling monomers
(amino-acids) with fixed
translation and rotation
Look for configurations
which have no steric
hindrance (i.e. clashes)
Calculate N-H…O=C
distances and
angles (3-d trigonometry..)
2 models satisfies all constraints
The α-helix – one of the two common
structural elements in proteins

N
C
O

i

i+4

Completes one turn every
3.7 residues
Rises ~5.4 Å with each
turn
Has hydrogen bonds
between the C=O of
residue i and the N-H of
residue i+4
Is right-handed
Alpha-helices appear a lot in transmembranal proteins
membrane
E.g. Lactose permease (LacY)
Why did Pauling and Corey succeed
where others failed?




Understanding the importance of hydrogen
bonds
Taking into account the planar peptide bond
Better knowledge of covalent bond lengths
and angles
MOST IMPORTANTLY – they were NOT
crystallographers, and did not consider only
models with integer number of residues per
turn!
Proof came 7 years later…
John Cowdery Kendrew
The Nobel Prize in Chemistry 1962
Kendrew, J. C., Bodo, G., Dintzis, H. M. Parrish, R. G., Wyckoff, H.,
and Phillips, D. C. A Three-Dimensional Model of the Myoglobin Molecule
Obtained by X-ray Analysis. Nature, 181, 662 (1958).
Hierarchy of Protein Structure
Linear chain made of 20 possible
amino acids
Alpha-helices, beta-sheets, turns
Motifs, domains
Oligomers, complexes
The Protein Data Bank (www.pdb.org)
The PDB contains over 40,000
structures (as of December 2006)
NMR - Nuclear magnetic resonance
Allows structure determination based on
distance and angular constraints in solution
Proteins’ Structure is Dynamic


Fluctuations exists in all proteins
Conformational changes ↔ Function
Adenylate kinase
An enzyme that catalyzes
the production of ATP from ADP
Protein Folding – still an open question

1954 Christian B. Anfinsen proved that the
protein structure is determined by it’s
sequence
Protein  Denatured (unfolded)  Protein
+ Urea
RNase
enzyme

Dilution
1969 “Levinthal paradox” – For a 100 a.a.
sequence there are 9100 possible
configurations. If sampled randomly every
nanosecond, it will take longer then the age
of the universe to fold a single protein
Protein folding – research continues

Late 1980’s - Wolynes et al. present the
“Energy Landscape” or “Folding Funnel” model
Entropy
for protein folding
Energy
Native
(folded) state

2006 – There is still no precise understanding
how proteins fold fast (up to µsec!), reliably and
accurately to their native structure