Structural Biology - Protein Crystallography Flashcards
What are the applications of studying protein structures?
Membrane proteins
Enzymes
Hormones
Nuclear receptors
Ion channels
Nucleic acids
Drug targets
Explore structure and function
Molecular basis of mutations and disease
Why a mutation is damaging the function of the protein
Explain the molecular basis of disease
Find mutations in the protein structure
Example a mutation that causes the pore to become more narrow
Therefore antibiotic couldn’t bind
Structure based drug design
Influenza drugs: Design of inhibitors to mimic binding of the substrate
COVID-19: Crystallise main protease of covid that facilitates viral transcription, Identify inhibitors of the protease - Idea for treatment before vaccines were created
What are X-Rays?
X-rays are in the range 10^-8 to 10^-12 nm wavelength
Small objects (molecules) need short wavelengths
Why can’t we use a microscope to see molecules?
Microscopes are used to see small objects
Only shows images of things with the same size as the wavelength of light (400-700nm)
Protein is 10nm big and atom is 0.1nm big so microscope can’t see a protein
X-rays have a similar wavelength to the size of an atom (0.1nm)
Can’t make X ray microscope due to it’s refractive index
How does X-ray crystallography work (basic)?
Grow crystals
Put crystal Infront of X-ray to create an X-ray diffraction pattern
Calculate electron cloud that surrounds an atom (electron density map)
Build model/protein structure
What is a crystal, molecule and atom?
Crystal:Ordered array of molecules in three dimensions (3D), many copies of molecules aligned in a specific order
Molecule: set of bonded atoms. The shape of a molecule is defined by the shape of the electron clouds associated with the constituent nuclei
Atom: nucleus (+ve) and electrons (-ve). Electron cloud surrounds the nucleus and is a lot larger than the nucleus of the atom. Volume and shape of atom is defined by the electron cloud. Electron cloud affects the shape of the crystal
A crystal is an ordered 3D array of distinctively-shaped distributions of electrons
X-ray as an electromagnetic wave
An X-ray is a travelling electromagnetic wave
There are oscillating electric (E) and magnetic (B) fields
E and B fields oscillate at right angles to each other and the direction of travel
E field: electrostatic force felt by a charged particle due to the presence/motions of other particles
Can be represented by a vector (a quantity with magnitude and direction)
Tells us which way a +ve charge will move
X-ray scattering by a single electron
X-ray (wave) is oscillating in an electric field (E)
Electron responds by oscillating
Oscillating electron is re-emitting X-rays over a wide angle (ripple effect)
Scattering of electric field from X-ray in ALL directions
X-ray scattering by two electrons
The scattering pattern (observed on the detector) is the result of adding the scattered waves
Waves of both electrons interact with each other
Resultant pattern depends on their relative position
Diffraction: When the X-ray has the same wavelength as the size of the molecule
The diffraction pattern depends on the structure
X-ray scattering by two electrons is like the two-slit experiment
Diffraction of water waves through 2 slits gives an unvarying pattern of peaks/troughs
Pattern depends on slit structure (width, separation) and the wavelength
The relationship between the diffraction pattern and slit structure can give us information of relative position of two atoms (how spaced out they are)
Explain circular/wave motion
360 Degrees = 2pi radians
Wave motion is cyclic - cosine and sine waves
Phase angle is the rotated position of line/where you are in the sine/cosine wave and it varies with x
Look at equation in notes
Waves have amplitude, phase and a defined wavelength
Adding waves - constructive interference
If two waves of amplitude A are perfectly in phase
(a peak in one wave = a peak in the other)
Then the phase difference is 2npi for n=1,2,3…
Resultant amplitude = 2A
Resultant has the same phase to the components
Adding waves - destructive interference
If two waves are perfectly out of phase
The phase difference = (2n-1)pi for n=1,2,3…
This will always give an odd number of p
The resultant amplitude = 0
Adding waves - intermediate example
2 waves that are partially out of phase
Phase difference is a fraction of 2pi
Resultant amplitude < 2A
Resultant has a different phase to the components
Amplitude and phase of the resultant wave depends on amplitude and phase of the components
How does X-ray scattering by two electrons in different positions affect the amplitude and phase shift?
Incident X-rays are in phase
X-ray interacts with the closest electron first and X-ray is scattered at angle of 2 theta
The second electron is further away, so X-ray travels longer
Results in a phase shift - two waves are out of phase
Amplitude is < 2A
Phase shift and amplitude is due to the structure
Scattering object is very small compared to distance to the detector - so rays from two objects can be assumed to be parallel
How is scattering from two electrons quantified in equations?
Use wave vectors (direction of wave vector = direction of travel)
K0 = incident wave vector (magnitude 1/l)
K = scattered wave vector (magnitude 1/l) at angle of 2theta
First electron (O) to be hit by the wave vector K0
To hit second electron (B), wave has to travel extra distance AB
R is a positional vector (gives information about position and length)
Use scattering vectors to work out the phase difference
Scattering vector (S) = K - K0
Length of S (|S|) = (2/lambda)sintheta
Triangle is isosceles so angles are equal
At fixed lambda (typical in experiments), |S| (amplitude of S) varies only with scattering angle
Phase difference between the ray scattered from O and the ray scattered from B (at position r): F = 2prS
So phase difference depends on:
r - the relative positions of the 2 electrons
S - the wavelength l and scattering angle theta
How are complex numbers used to transform the wave equation?
Wave equation becomes Y=Ae^(i*F)
I is an imaginary number
It is a negative number that stays negative when squared
Wavelength is constant in experiment, so can look only at the phase shift
What is the structure factor, f(S)?
Mathematical equation of the diffraction pattern
Describes how the diffracted waves in each direction are related to the structure (the positions of the electrons, r)
It is a wave: has an amplitude and phase
It is a complex number since it is a sum of complex numbers
Longer equation (in notes):
S = scattering vector (depends on angles and wavelengths of incident and diffracted X-rays)
N = number of atoms in unit cell
j = adding new wave in order of 1 (increasing wave by one each time)
R = positional vector
I = imaginary unit
Can be shortened to: f(S) =|f(S)|e^(iF(S))
Shows amplitude (two parallel lines) and phase (e^i)
Explain how multiple electrons interact to give amplitude and phase
Multiple scattered waves of the same amplitude going in direction 2 theta
Phase of each depends on the position of the electron it scattered from
Gives a new resultant wave: a new amplitude and new phase
Amplitude and phase depends on the amplitude and phase of the components
What is electron density and the electron density function?
In an atom/molecule the positions of the electrons are not well defined
There is an electron cloud around the nucleus
These are the electrons that will interact with the X-rays
Distribution of electrons is described by a 3D electron density function r (r ) = r (x,y,z)
At position r in the molecule there is an amount of electron density: r (r ) = dxdydz
Where dxdydz is an infinitesimally small cube (volume)
Electron density function tells us the probability of finding electrons in that position (r position)
For a single atom, the highest electron density is in the middle
f ( S ) = mathematical equation of describing scattering on detector
r ( r ) = electron density in the molecule
Scattering by a molecule in direction, S
Every part of the molecule scatters in every direction
Consider all the scattering in just ONE direction, S (at an angle of 2theta)
Amplitude is proportional to the electron density function as it depends on where the x-rays are coming from
Amplitude assumed to be one before but now defined by electron density function
Electron density is higher in the core of the molecule and lower at the edges
Structure factor for multi-electron system: f(S) =|f(S)|e^I(2pir(S))
Structure factor for molecule: f(S) = integral (r(r)dxdydz) e^I(2pir(S))
Now integrating in XYZ (3-dimensions) because there is so many points (assume infinity)
Add up contributions to find total scattering in one direction
If have different angle of scattering, value of f(S) is different because amplitude is different (because phases are different or less electrons are interacting)
Some dots on result are darker, some lighter
Fourier transform to measure scattering
The total scattering in the direction (S) from an object ( r (r ) ) is the sum of the waves scattered from every point in the object
Measuring addition of all the waves coming from all the atoms within the molecule
Look at equation in notes
Inverse Fourier transform to measure scattering
Inverse Fourier transform: used to determine the real structure r ( r ) from diffraction pattern f ( S)
We have to measure the scattering in all directions (at all values of S to work out the structure, r ( r )
Rotate the molecule by 2theta every time
The theory works for any structure
Why are crystals used instead of single molecules?
Individuals molecules give a weak signal that is hard to distinguish from the background noise of the detector. They scatter very few photons
Crystals contain billions of molecules. They amplify the scattering, making it detectable. Properties of crystals restrict scattering to certain directions
In a crystal: orientation of all molecules is the same –> all waves are added together –> constructive interference –> strong signal on the detector
Explain the properties of crystals and what a unit cell is
There are huge numbers of molecules in a crystal
Crystal = 0.2mm, Molecule = 10nm
So there is 20,000 molecules along one side and 8,000,000,000,000 in total
Repetitive nature: each molecule is aligned in the same direction
Each molecule occupies a unit cell
A unit cell is the smallest repeating unit of the crystal with translational symmetry (like a brick)
Unit cells can have more than one molecule
Crystals have many unit cells
Reflection of X-rays from a semi-transparent layer of molecules
Crystal planes are semi-transparent
Only 2% of X-rays are scattered from a protein crystal
So each layer of molecules in the crystal scatters far less
Every plane contributes more or less equally to the scattering from the crystal
Crystals are made of several layers
X-rays penetrate every crystal layer and every layer diffracts the X-ray which amplifies the signal
Diffracted x-rays interfere between layers but signal is not strong enough to measure
Explain Bragg’s law
Incident angle theta(i) and reflected angle theta(r) are equivalent
Path difference = 2dsin(theta)
Bragg’s Law: Strong diffraction if path difference is a whole number of wavelength
2dsin(theta) = n(lambda)
n = integer/whole number
d = spacing between crystals
If the two layers are in phase, there is strong interference
Explain Bragg’s law with destructive interference
Different incident angle
2dsin(theta) = (2n-1)lambda/2, where 2n-1 is odd
When path difference is an odd number of half a wavelength
Leads to destructive interference
No scattering on the detector
Applies to layers of a crystal:
At layer 1: path difference is almost a whole number (will see diffraction)
At layer 50: wavelength is an odd number of half a wavelength which doesn’t obey bragg’s law
Destructive interference and no diffraction
Last layers could give a diffraction
How are layers in crystals connected?
Layers connected via H-bonds, salt bridges, hydrophobic interactions
Crystalline lattice connected in different dimensions (3D)
Molecular vs Crystalline scattering
Single molecule:
Diffraction pattern is related to the structure but too weak to detect in practice
Diffraction is too weak to distinguish from background of detector
Background noise of detector due to scattering of air
Signal to noise ratio is very low
Crystalline:
Much higher signal to noise ratio
Diffraction spots are clearly distinguished from the background scatter
Diffraction pattern is the same as that for the molecule but only observed in particular directions (made up of spots)
Explain how crystalline diffraction works
Scattering only occurs if the path difference between waves from adjacent layers is a whole wavelength
Law is effective because there are huge numbers of molecules in a crystal (20,000 molecules along one side)
Crystalline samples amplify the scattered intensity
Makes it measurable in allowed directions
The positions of observed rays tells us about the orientation and spacing of the planes within the crystals
The variation in intensity (spots/reflections) is the same as the variation you would see in a single molecule
Some areas have no diffraction (no black spots on detector) due to destructive interference or weak electron density