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Лекция 4+5 Другие методы исследования структуры белков (SAXS/SANS, Cryo-EM,

Содержание

Small-angle X-ray scattering (SAXS) + Small-angle neutron scattering (SANS) II Small-angle scattering (SAS)

Слайды и текст этой презентации

Слайд 1Лекция 4+5 Другие методы исследования структуры белков (SAXS/SANS, Cryo-EM, Cryo-electrotomography, NMR,

native-MS, crosslinking MS, HDX-MS). Интегральный подход и моделирование белков по

гомологии (iTasser). Примеры.

Случанко Н.Н.

Лекция 4+5  Другие методы исследования структуры белков (SAXS/SANS, Cryo-EM, Cryo-electrotomography, NMR, native-MS, crosslinking MS, HDX-MS). Интегральный

Слайд 2Small-angle X-ray scattering (SAXS) + Small-angle neutron scattering (SANS) II Small-angle scattering (SAS)

Small-angle X-ray scattering (SAXS) + Small-angle neutron scattering (SANS) II Small-angle scattering (SAS)

Слайд 3SAXS popularity
Blanchet C. (c)

SAXS popularityBlanchet C. (c)

Слайд 4Основы SAS
~1 photon in 106 incident photons

Основы SAS~1 photon in 106 incident photons

Слайд 5Основы SAS
s and q are just alternative designations of the

scattering vector,
usually from 0 to 0.5 Å-1
~ 10-20 Å

Основы SASs and q are just alternative designations of the scattering vector, usually from 0 to 0.5

Слайд 6Contrast and careful buffer subtraction
Measured in the same cell, buffer

exactly matches
Difference in the scattering density (contrast):

Contrast and careful buffer subtractionMeasured in the same cell, buffer exactly matchesDifference in the scattering density (contrast):

Слайд 7Kikhney A (c)
Processed final curve !

Kikhney A (c)Processed final curve !

Слайд 8Особенности
Макромолекулы свободно вращаются, не ориентированы строго при падающем пучке X-ray
Может

быть несколько конформаций одновременно
В результате наблюдаемое рассеяние это сферическое усреднение

(изотропное) и усреднение по времени
Теряется 3D информация
Данные при радиальном усреднении дают 1D кривую распределения I(q) с небольшим числом параметров

Данные – 1D кривая…

ОсобенностиМакромолекулы свободно вращаются, не ориентированы строго при падающем пучке X-rayМожет быть несколько конформаций одновременноВ результате наблюдаемое рассеяние

Слайд 10https://www.embl-hamburg.de/biosaxs/software.html

https://www.embl-hamburg.de/biosaxs/software.html

Слайд 11Форма кривой SAXS сильно зависит от размера и формы частиц

Форма кривой SAXS сильно зависит от размера и формы частиц

Слайд 12What does the curve already tell us about the size

of the particles? What is the resolution?
s, nm-1
logI
d ~ 1.4

nm
What does the curve already tell us about the size of the particles? What is the resolution?s,

Слайд 13Pairwise distance distribution function p(r)
Blanchet C. (c)
FFT

Pairwise distance distribution function p(r)Blanchet C. (c)FFT

Слайд 14Pairwise distance distribution function p(r)
Blanchet C. (c)
FFT
Dmax
maximum intra-particle distance

Pairwise distance distribution function p(r)Blanchet C. (c)FFTDmaxmaximum intra-particle distance

Слайд 16Kikhney A (c)
DAMMIF program
https://www.embl-hamburg.de/biosaxs/dammif.html

Kikhney A (c)DAMMIF programhttps://www.embl-hamburg.de/biosaxs/dammif.html

Слайд 20Linear ≠ monodisperse
(also for mixed systems)

Linear ≠ monodisperse(also for mixed systems)

Слайд 21Guinier plot and Rg
Average of square center-of-mass distances in the

molecule
Measure of the overall size of the molecule
R
A. Guinier

Guinier plot and RgAverage of square center-of-mass distances in the moleculeMeasure of the overall size of the

Слайд 22Kratky plot and flexibility
Identification of unfolded samples
Globular proteins have bell-shaped

curves (parabola)

Kratky plot and flexibilityIdentification of unfolded samplesGlobular proteins have bell-shaped curves (parabola)

Слайд 23If X-ray structures are available…
Atomistic modeling:
Validation of the crystal structure

against solution situation
Rigid-body fitting
Missing fragments (loops)
Conformational transitions
Theoretical SAXS profile can

be calculated by CRYSOL program, necessary for fitting
If X-ray structures are available…Atomistic modeling:Validation of the crystal structure against solution situationRigid-body fittingMissing fragments (loops)Conformational transitionsTheoretical

Слайд 24Validation of the crystal structure in solution situation
1.75A

Validation of the crystal structure in solution situation1.75A

Слайд 25Comparison of the crystal structures and ab initio envelopes

Comparison of the crystal structures and ab initio envelopes

Слайд 26Conformational change

Conformational change

Слайд 27Conformational change
FRP dimer

Conformational changeFRP dimer

Слайд 28SEC-SAXS for contaminated samples
M. Graewert (c)

SEC-SAXS for contaminated samplesM. Graewert (c)

Слайд 29SASBDB https://www.sasbdb.org/aboutSASBDB/

SASBDB https://www.sasbdb.org/aboutSASBDB/

Слайд 30 Трезвый взгляд на SAXS
Дает хорошую информацию о гидродинамических свойствах

частиц (структурных свойствах) в растворе
Хорош для тестирования гипотез о структуре,

форме, комплексе и т.п.
Вспомогательный метод структурной биологии
Необходимо сверяться с как можно большим количеством экспериментальных данных (стехиометрия, олигомерное состояние, размеры, масса, радиус, пространственные ограничения, знания об интерфейсах, топологии субъединиц и т.п.)
В одиночку SAXS не стоит использовать для структурной биологии (ambiguity)
Трезвый взгляд на SAXSДает хорошую информацию о гидродинамических свойствах частиц (структурных свойствах) в раствореХорош для тестирования

Слайд 31SANS
Neutron source (rare)
Non-ionizing radiation
Coherent scattering (=elastic)
Incoherent scattering (1H affects)
Contrast is

very different in H2O and D2O
SAXS and SANS are complementary!
Contrast

variation by increasing D2O content:

Difference in the scattering density (contrast)

Study of conformational changes of selected proteins within the complexes !!!

Features:

SANSNeutron source (rare)Non-ionizing radiationCoherent scattering (=elastic)Incoherent scattering (1H affects)Contrast is very different in H2O and D2OSAXS and

Слайд 32Samples for SAXS and SANS

Samples for SAXS and SANS

Слайд 33CryoEM
https://www.nature.com/news/the-revolution-will-not-be-crystallized-a-new-method-sweeps-through-structural-biology-1.18335
https://www.youtube.com/watch?v=aHhmnxD6RCI

CryoEMhttps://www.nature.com/news/the-revolution-will-not-be-crystallized-a-new-method-sweeps-through-structural-biology-1.18335 https://www.youtube.com/watch?v=aHhmnxD6RCI

Слайд 34Resolution revolution
появление прямых детекторов электронов
развитие софта для обработки огромного количества

картинок
совершенствование микроскопов, адаптация к криоусловиям

Resolution revolutionпоявление прямых детекторов электроновразвитие софта для обработки огромного количества картиноксовершенствование микроскопов, адаптация к криоусловиям

Слайд 35The recipe includes
https://www.youtube.com/watch?v=BJKkC0W-6Qk

The recipe includeshttps://www.youtube.com/watch?v=BJKkC0W-6Qk

Слайд 36The process of Cryo-EM single particle analysis technique
by cross-correlation

The process of Cryo-EM single particle analysis techniqueby cross-correlation

Слайд 37Features, 2D->3D
Biological samples – low doses and dehydration (high vacuum)
Freezing

allows to avoid these, but the images have a very

low contrast
Each picture - 2D projection of a 3D object
Multiple 2D projections can be used to reconstruct the 3D object

DOI: 
10.1142/9781848164666_0001

http://www.ejectamenta.com/Imaging-Experiments/fourierimagefiltering.html

Features, 2D->3DBiological samples – low doses and dehydration (high vacuum)Freezing allows to avoid these, but the images

Слайд 38Contrast transfer function and defocus
At perfect focus, biological specimens produce

little contrast in vitreous ice.
To produce phase contrast, pictures are

taken underfocus, at the expense of systematic alteration of the image data (not all waves are well transferred -> CTF)
Each picture is undergoing FT to see Thon rings (~resolution rings in Xtallography) – contrast transfer function (CTF)
Some waves are lost but can be CTF-corrected upon changing defocus (d below)

Contrast transfer function and defocusAt perfect focus, biological specimens produce little contrast in vitreous ice.To produce phase

Слайд 39Contrast transfer function and defocus
At perfect focus, biological specimens produce

little contrast in vitreous ice.
To produce phase contrast, pictures are

taken underfocus, at the expense of systematic alteration of the image data (not all waves are well transferred -> CTF)
Each picture is undergoing FT to see Thon rings (~resolution rings in Xtallography) – contrast transfer function (CTF)
Some waves are lost but can be CTF-corrected upon changing defocus (d below)

d is varied

Contrast transfer function and defocusAt perfect focus, biological specimens produce little contrast in vitreous ice.To produce phase

Слайд 40Contrast transfer function and defocus
DOI: 10.1142/9781848164666_0001

Contrast transfer function and defocusDOI: 10.1142/9781848164666_0001

Слайд 41Single particle cryoEM requires tons of images
Particle orientations are classified

by cross-correlation
Each class should be represented by thousands of images
Also,

at different defocus values
Some images are discarded
Single particle cryoEM requires tons of imagesParticle orientations are classified by cross-correlationEach class should be represented by

Слайд 42Signal and noise
5:1
1:1
S/N = 1:1 (0 dB)
Improving S/N by repetition

and averaging
4 measurements = 2 *S/N
50S ribosome projection
Accurate alignment and

the target model are important
Signal and noise5:11:1S/N = 1:1 (0 dB)Improving S/N by repetition and averaging4 measurements = 2 *S/N50S ribosome

Слайд 43Einstein from noise
An image of Einstein appears from averaged 1000

images of pure white noise by using a normalized cross-correlation

function and the photo as a model.

doi: 10.1016/j.jsb.2008.12.008

Einstein from noiseAn image of Einstein appears from averaged 1000 images of pure white noise by using

Слайд 44Обучение криоЭМ
https://ru.coursera.org/learn/cryo-em
https://em-learning.com
https://www.youtube.com/watch?v=Bk5lBvwSe-s
Prof. Yifan Cheng

Обучение криоЭМhttps://ru.coursera.org/learn/cryo-emhttps://em-learning.com https://www.youtube.com/watch?v=Bk5lBvwSe-s Prof. Yifan Cheng

Слайд 46Cryo-electrotomography (Cryo-ET)

Cryo-electrotomography (Cryo-ET)

Слайд 47Cryo-electrotomography (Cryo-ET)
https://doi.org/10.1371/journal.pbio.3000050

Cryo-electrotomography (Cryo-ET)https://doi.org/10.1371/journal.pbio.3000050

Слайд 48NMR – nuclear magnetic resonance
https://www.youtube.com/watch?v=0s7Cbl8bZLM
https://www.youtube.com/watch?v=eY0NyE0SQjE 
NMR made super easy:

NMR – nuclear magnetic resonancehttps://www.youtube.com/watch?v=0s7Cbl8bZLMhttps://www.youtube.com/watch?v=eY0NyE0SQjE  NMR made super easy:

Слайд 49The output of the (successful) multidimensional NMR experiment
A set of

structural models that satisfy the experimental constraints but also obey

the chemistry rules
The output of the (successful) multidimensional NMR experimentA set of structural models that satisfy the experimental constraints

Слайд 50NMR
Spin up
Or
Spin down
https://www.youtube.com/watch?v=PmYwYUQw-Rw

NMRSpin up OrSpin downhttps://www.youtube.com/watch?v=PmYwYUQw-Rw

Слайд 51Properties of some nuclei
Bonvin A (c)

Properties of some nucleiBonvin A (c)

Слайд 52NMR sample
Bonvin A (c)

NMR sampleBonvin A (c)

Слайд 53Bonvin A (c)
Nuclear spin
Частота прецессии (Ларморова частота)

Bonvin A (c)Nuclear spinЧастота прецессии (Ларморова частота)

Слайд 54Energy between α (+1/2) and β (-1/2) levels
1H

Energy between α (+1/2) and β (-1/2) levels1H

Слайд 55Transitions between levels are possible

Transitions between levels are possible

Слайд 56NMR, a spectroscopy technique
In a magnetic field magnetic nuclei will

resonate with a specific frequency

NMR, a spectroscopy techniqueIn a magnetic field magnetic nuclei will resonate with a specific frequency

Слайд 57Bonvin A (c)

Bonvin A (c)

Слайд 58Magnetization (M) gets back to the B0-oriented position after being

affected by external field
B0
Exponential decay
Free induction decay (FID)
Relaxation
=спад свободной индукции

Magnetization (M) gets back to the B0-oriented position after being affected by external fieldB0Exponential decayFree induction decay

Слайд 59Chemical shift due to the local environment changing frequency of

the nuclei
Expressed as part per million (ppm) by comparison to

the reference frequency:

(may also be presented in Hz)

Chemical shift due to the local environment changing frequency of the nucleiExpressed as part per million (ppm)

Слайд 60The local electronic environment of the nucleus may change the

frequency: shielding effect
resonances
deshielding
shielding

The local electronic environment of the nucleus may change the frequency: shielding effectresonancesdeshieldingshielding

Слайд 61Pulse method to deliver a set of ν and then

do …
Good old Fourier !

Pulse method to deliver a set of ν and then do …Good old Fourier !

Слайд 621D 1H-spectrum of ethanol
CH3–CH2–OH
(CH3)4Si
Chemical shift
Several peaks due to spin-spin interaction

1D 1H-spectrum of ethanolCH3–CH2–OH(CH3)4SiChemical shiftSeveral peaks due to spin-spin interaction

Слайд 632D spectra
Series of pulses to cause transitions
2D Fourier transformation
Proximal functional

groups affect the magnetization of a particular nucleus in the

structure
2D spectraSeries of pulses to cause transitions2D Fourier transformationProximal functional groups affect the magnetization of a particular

Слайд 64Спектр 15N-1H HSQC apo-CTDH (0.5 mM), при 800 MHz и

35°С. Отнесены сигналы амидных групп белковой цепи.
ApoCTDH
6FEJ.pdb
http://pdbflex.org/index.html
Наложение спектров 15N-1H

HSQC apo-CTDH (красные) и CTDH-Canthaxanthin (синие)

K14
A17
L31
P36
G56
G59
L67
G97
V108
F112
H122

Спектр 15N-1H HSQC apo-CTDH (0.5 mM), при 800 MHz и 35°С. Отнесены сигналы амидных групп белковой цепи.ApoCTDH6FEJ.pdbhttp://pdbflex.org/index.html

Слайд 65Resolution of the peaks is increased upon increasing dimensionality

Resolution of the peaks is increased upon increasing dimensionality

Слайд 66Structural models of small proteins
Distances between neighboring atoms
Angles ψ and

φ of the polypeptide chain
2MOU.pdb
STARD6
20 structures

Structural models of small proteinsDistances between neighboring atomsAngles ψ and φ of the polypeptide chain2MOU.pdbSTARD620 structures

Слайд 67NMR tackles both structured proteins and IDPs

NMR tackles both structured proteins and IDPs

Слайд 68NMR tackles both structured proteins and IDPs

NMR tackles both structured proteins and IDPs

Слайд 69i-Tasser. Protein structure prediction
FASTA format of sequence
https://zhanglab.ccmb.med.umich.edu/I-TASSER/

i-Tasser. Protein structure predictionFASTA format of sequencehttps://zhanglab.ccmb.med.umich.edu/I-TASSER/

Слайд 70Comparison of different structural techniques

Comparison of different structural techniques

Слайд 71Integrated approaches in structural biology
X-ray crystallography
SAXS
NMR
CryoEM
Auxillary techniques: fluorescence resonanse energy

transfer (FRET), limited proteolysis, native-MS, crosslinking, HDX, molecular dynamics and

computational biology
Integrated approaches in structural biologyX-ray crystallographySAXSNMRCryoEMAuxillary techniques: fluorescence resonanse energy transfer (FRET), limited proteolysis, native-MS, crosslinking, HDX,

Слайд 72Native-MS
https://doi.org/10.3389/fmicb.2018.01397

Native-MShttps://doi.org/10.3389/fmicb.2018.01397

Слайд 73Native-MS
https://doi.org/10.1007/s13361-018-2061-4
highly charged complexes
no additional charges
https://www.nature.com/articles/nmeth.1265
https://www.pnas.org/content/116/4/1116
DOI: 10.1007/978-1-4939-7151-0_11

Native-MShttps://doi.org/10.1007/s13361-018-2061-4highly charged complexesno additional chargeshttps://www.nature.com/articles/nmeth.1265 https://www.pnas.org/content/116/4/1116 DOI: 10.1007/978-1-4939-7151-0_11

Слайд 74Hydrogen/deuterium exchange mass-spectrometry
Yoshitomo Hamuro ©
0°C, H+
https://doi.org/10.1016/j.sbi.2019.06.007
https://onlinelibrary.wiley.com/doi/abs/10.1002/pro.3790
amide protons

Hydrogen/deuterium exchange mass-spectrometryYoshitomo Hamuro ©0°C, H+https://doi.org/10.1016/j.sbi.2019.06.007https://onlinelibrary.wiley.com/doi/abs/10.1002/pro.3790 amide protons

Слайд 75Pseudoatomic models built by a combination of:
Single particle Cryo-EM
Crosslinking MS
HDX

MS
Modelling

Pseudoatomic models built by a combination of:Single particle Cryo-EMCrosslinking MSHDX MSModelling

Слайд 76Cryo-EM micrograph of human alphaA-crystallin
12-mer
16-mer
20-mer

Cryo-EM micrograph of human alphaA-crystallin12-mer16-mer20-mer

Слайд 77Cryo-EM 3D reconstructions of human αA-crystallin (reduced) oligomers
Scale bar,

10 nm
239 kDa
319 kDa
398 kDa

Cryo-EM 3D reconstructions of human αA-crystallin (reduced) oligomers Scale bar, 10 nm239 kDa319 kDa398 kDa

Слайд 78Crosslinking by BS3 and MS
Fragmentation spectrum of a cross-linked peptide

with an intramolecular link between K70 and K99
Fragmentation spectrum

of a cross-linked
peptide with an intermolecular cross-link between M1 and M1

bis(sulfosuccinimidyl)suberate (BS3)

11.4A

Crosslinking by BS3 and MSFragmentation spectrum of a cross-linked peptide with an intramolecular link between K70 and

Слайд 79Pseudoatomic model of the 16-mer
Modelling by molecular dynamics flexible fitting

was based on:
-shape, symmetry and low-resolution features from 9-10 Å

resolution Cryo-EM maps
-crystal structures of truncated versions (domains)
-crosslinking MS data (pairs of residues located within certain distance)
-stereochemistry restraints

Pseudoatomic model of the 16-merModelling by molecular dynamics flexible fitting was based on:-shape, symmetry and low-resolution features

Слайд 80Effect of alphaA-crystallin oxidation
Far-UV CD
Near-UV CD
anSEC
AUC-SV
14S
25S
50nm
50nm
Negative stain TEM

Effect of alphaA-crystallin oxidationFar-UV CDNear-UV CDanSECAUC-SV14S25S50nm50nmNegative stain TEM

Слайд 81HDX-MS shows incresed local structural dynamics of alphaA-crystallin
Deuteration uptake behavior

of the oxidized and reduced αA
Difference in local relative deuterium

uptake (ΔD uptake αAox − αAred)
HDX-MS shows incresed local structural dynamics of alphaA-crystallinDeuteration uptake behavior of the oxidized and reduced αADifference in

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