Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture...

13
Determination of the image orientation E. Orlova Lecture 11 Images: shadow, projection, Euler angles Methods of orientation determination: Projection matching: Real space & Polar Fourier coordinates Common lines in Fourier space Common lines in real space FREALIGN (Fourier REconstruction and ALIGNment) Practical Course Birkbeck College London Image processing for cryo microscopy Sep 5 - Sept 15, 2017 Images of molecules in vitreous ice Images ---??--- Object surface view, shadow, projection Object Photograph = surface view Projection Projection X-ray picture Shadow Shadow (positive) Shadow (negative)

Transcript of Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture...

Page 1: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Det

erm

inat

ion

of

the

imag

e or

ient

atio

n

E. O

rlova

Le

ctur

e 11

Imag

es: s

hado

w, p

roje

ctio

n, E

uler

ang

les

Met

hods

of o

rient

atio

n de

term

inat

ion:

P

roje

ctio

n m

atch

ing:

R

eal s

pace

& P

olar

Fou

rier c

oord

inat

es

Com

mon

line

s in

Fou

rier s

pace

C

omm

on li

nes

in re

al s

pace

F

REA

LIG

N (F

ourie

r REc

onst

ruct

ion

an

d AL

IGN

men

t)

Pra

ctic

al C

ours

e

Birk

beck

Col

lege

Lo

ndon

Imag

e pr

oces

sing

fo

r cry

o m

icro

scop

y

Sep

5 - S

ept 1

5, 2

017

Imag

es o

f mol

ecul

es i

n vi

treo

us ic

e

Im

ages

---?

?---

Obj

ect

sur

face

vie

w,

sha

dow

, pr

ojec

tion

Obj

ect

Phot

ogra

ph =

su

rfac

e vi

ew

Proj

ectio

n Pr

ojec

tion

ojec

toX

-ray

pic

ture

Shad

ow

Shad

ow(p

ositi

ve)

Shad

ow

(neg

ativ

e)

Page 2: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

3D

obj

ect

->

(x,y,

z)

Proj

ectio

n: 2

D, 1

D, S

inog

ram

= ?

=

(x,y

,z)

dxz

yx

zy

p)

,,

()

,(

dxy

xp

yl

),

()

(p(y,z

) – 2

D p

roje

ctio

n

l(y) –

1D

pro

ject

ion

Rib

osom

es in

vitr

eous

ice

– tra

nsla

tiona

l fre

edom

X

y X

and

Y

2

J.Fr

ank,

Ann

u. R

ev. B

ioph

ys. B

iom

ol. S

truct

. 200

2. 3

1:30

3–19

Rib

osom

es in

vitr

eous

ice

– ro

tatio

nal f

reed

om

and

→ 3

(IMAG

IC)

- ro

tatio

n in

th

e im

age

plan

e

(or a

roun

d ne

w

Z ax

is)

- ro

tatio

n ar

ound

X a

xis

– ro

tatio

n

arou

nd o

ld

Z a

xis)

Page 3: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Leon

hard

Eul

er

http

://en

.wik

iped

ia.o

rg/w

iki/L

eonh

ard_

Eule

r

Eule

r sp

ent

mos

t of

his

adu

lt lif

e in

St.

Pete

rsbu

rg,

Rus

sia,

an

d in

Be

rlin,

Pr

ussi

a.

He

is

the

pre-

emin

ent

mat

hem

atic

ian

of t

he 1

8th

cent

ury,

and

on

e of

the

grea

test

mat

hem

atic

ians

eve

r. hi

s co

llect

ed

wor

ks

fill

60–8

0 qu

arto

vo

lum

es

(15

April

170

7 –

18 S

epte

mbe

r 178

3)

was

a

pion

eerin

g Sw

iss

mat

hem

atic

ian

and

phys

icis

t. H

e m

ade

impo

rtant

dis

cove

ries

in f

ield

s as

div

erse

as

infin

itesi

mal

cal

culu

s an

d gr

aph

theo

ry. H

e al

so in

trodu

ced

muc

h of

the

mod

ern

mat

hem

atic

al

term

inol

ogy

and

nota

tion,

He

is a

lso

reno

wne

d fo

r hi

s w

ork

in m

echa

nics

, flu

id

dyna

mic

s,

optic

s,

and

astro

nom

y.

Met

hods

of o

rient

atio

n de

term

inat

ion:

1.

Con

ical

Tilt

– M

.Rad

erm

ache

r, J.

Fra

nk

2.P

roje

ctio

n M

atch

ing

– P.

Penc

zek,

J.F

rank

3.

Pol

ar F

ourie

r Tra

nsfo

rm –

T. B

acke

r 4.

Com

mon

Lin

es in

Fou

rier S

pace

(viru

ses,

ph

age

tails

) T.C

row

ther

- MR

C p

acka

ge +

nu

mer

ous

mod

ifica

tion

(S. F

ulle

r) 5.

Com

mon

Lin

es in

real

spa

ce

Ang

ular

Rec

onst

itutio

n, M

. Van

Hee

l 6.

Frea

lign

-> p

roje

ctio

n m

atch

ing

in F

ourie

r sp

ace

, N. G

rigor

ieff

Con

ical

tilt

, mor

e ef

fect

ive

for n

egat

ivel

y st

aine

d sa

mpl

es

RA

DER

MA

CHER

M. T

hree

-Dim

ensi

onal

Rec

onst

ruct

ion

of S

ingl

e Pa

rticl

es

From

Ran

dom

and

Non

rand

om T

ilt S

erie

s. J

OU

RN

AL

OF

ELE

CTR

ON

M

ICR

OS

CO

PY

TEC

HN

IQU

E 9

:359

-394

(198

8)

Con

ical

tilt

Page 4: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Proj

ectio

n M

atch

ing

P. P

encz

ek &

J. F

rank

Proj

ectio

n M

atch

ing

P. P

encz

ek &

J. F

rank

PFT

Met

hod:

Th

ere

is a

noth

er w

ay to

hel

p de

term

ine

and

refin

e or

igin

and

vie

w o

rient

atio

n pa

ram

eter

s fo

r 3D

R s

tudi

es

PFT

= Po

lar F

ourie

r Tra

nsfo

rm EM

PFT

Hel

ps d

eter

min

e (

,x,y

) for

cry

oEM

imag

es

of p

artic

les

with

icos

ahed

ral s

ymm

etry

From

Tim

Bak

er

Asym

met

rical

tria

ngle

for s

ymm

etry

532

Page 5: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

BPV

Proj

ectio

ns: 1

/2 Ic

osah

edra

l ASU

0 3

6 9

12

15

18

21

24

27

30

90

87

84

81

78

75

72

69

From

Tim

Bak

er

EMPF

T

r (ra

dius

)

r

(azi

mut

hal a

ngle

)

Com

pute

Pol

ar P

roje

ctio

ns

Car

tesi

an

Pola

r

From

Tim

Bak

er

EMPF

T

Com

pute

Pol

ar F

ourie

r Tra

nsfo

rm

r (ra

dius

)

(azi

mut

hal a

ngle

) (s

patia

l fre

quen

cy)

Pola

r Pro

ject

ion

Pola

r FT

(Rea

l + R

ecip

roca

l)

From

Tim

Bak

er

Com

pute

Pol

ar F

ourie

r Tra

nsfo

rm

EMPF

T

5F

5F

Rea

l Dat

a Fr

om

Tim

Bak

er

Page 6: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

The

sect

ion/

proj

ectio

n th

eore

m:

F [

g(x,

y,z)d

x ] =

G(0

,Y,Z

)

USE

: Th

e Fo

urie

r tra

nsfo

rm o

f a p

roje

ctio

n of

a 3

D o

bjec

t is

equa

l to

a ce

ntra

l sec

tion

of th

e 3D

Fou

rier t

rans

form

of t

he o

bjec

t. An

ele

ctro

n m

icro

grap

h is

a p

roje

ctio

n of

a 3

D o

bjec

t. Its

tran

sfor

m p

rovi

des

one

slic

e of

the

3D tr

ansf

orm

of t

he 3

D

obje

ct.

By c

ombi

ning

the

trans

form

s of

diff

eren

t vie

ws,

one

bui

lds

up

the

3D tr

ansf

orm

sec

tion

by s

ectio

n. O

ne th

en u

ses

the

Inve

rsed

Fou

rier T

trans

form

to

conv

ert t

he 3

D tr

ansf

orm

into

a

3D im

age.

Com

mon

line

s in

Fou

rier s

pace

Com

mon

line

s in

Fou

rier s

pace

From

S F

ulle

r

Icos

ahed

ral s

ymm

etry

, se

arch

for t

he c

omm

on li

nes

Com

paris

on o

f am

plitu

des

and

ph

ases

of r

adia

l lin

es,

asse

ssm

ent o

f ang

les

betw

een

them

Page 7: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

An o

rient

atio

n aw

ay fr

om s

ymm

etry

axe

s

2 5

5

3

From

S F

ulle

r

Com

mon

line

s in

real

spa

ce

The

angu

lar r

econ

stitu

tion

met

hod

is

base

d on

the

“com

mon

-line

pro

ject

ion”

th

eore

m:

Any

two

2D p

roje

ctio

ns o

f a 3

D o

bjec

t ha

ve a

t lea

st O

NE

com

mon

1D

line

pr

ojec

tion

3D

2D

1

D p

roje

ctio

n

3D o

bjec

t y

x

z

dxz

yx

zy

p)

,,

()

,( p(

y,z)

2D p

roje

ctio

n

z

2Dy

Com

mon

line

s in

real

spa

ce

Com

mon

line

s in

real

spa

ce

Page 8: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Com

mon

line

s in

real

spa

ce

Com

mon

line

s in

real

spa

ce

Com

mon

line

s in

R/F

(our

ier)

spac

e Co

mm

on li

nes

in R

/F(o

urie

r) sp

ace

Page 9: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Com

mon

line

s in

R/F

(our

ier)

spac

e

2D

1D

2D p

roje

ctio

n

Sino

gram

is a

set

of

one

dim

ensi

onal

(li

ne) p

roje

ctio

ns

y

00

a

360

0

Com

mon

line

s in

real

spa

ce

900

880

920

2700

2720

2680

450

750

900

1400

1830

2700

3200

Proj

ectio

ns >

Sin

ogra

ms

0 o

360 o

180 o

0 o

360 o

180 o

25 o

50 o

50 000000000000o

90 000000000000o

25 55555o

25 555o

90 o

90 o

0 o

90 o

90 o

90 o

0 o 0 o

0 o

360 o

180 o

90 o

130 o

65 o

270 o

310 o

335 o

Page 10: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Cro

ssin

ocor

rela

tion

func

tion

Imag

e 2

Imag

e 1

-6-4-202468

111

2131

4151

6171

8191

101

111

121

-6-4-202468

111

2131

4151

6171

8191

101

111

121

Cro

ssin

ocor

rela

tion

func

tion

Imag

e 3

Imag

e 1

-6-4-20246

111

2131

4151

6171

8191

101

111

121

-6-4-20246

111

2131

4151

6171

8191

101

111

121

-6-4-20246

111

2131

4151

6171

8191

101

111

121

900

2700

3100

1300

Cro

ssin

ocor

rela

tion

func

tion

Imag

e 3

Imag

e 2

-6-4-202468

111

2131

4151

6171

8191

101

111

121

-6-4-202468

111

2131

4151

6171

8191

101

111

121

a b

c

d e

f

g

Proj

ectio

ns 1

and

3

Rib

osom

e A

ngul

ar R

econ

stitu

tion

Page 11: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

a b'

c

d'

e'

f'

g'

Proj

ectio

ns 2

and

3

Rib

osom

e A

ngul

ar R

econ

stitu

tion

Com

mon

line

s

AN

GU

LA

R R

EC

ON

STIT

UT

ION

Cal

cium

rele

ase

chan

nel

RyR

1

Cro

ssin

ocor

rela

tion

func

tion

Icos

ahed

ral s

ymm

etry

Imag

e 1

Imag

e 2

Page 12: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Dis

tribu

tion

of c

hara

cter

istic

vie

ws

- C

6 H

SV-1

FREA

LIG

N

(Fou

rier R

econ

stru

ctio

n an

d A

LIG

Nm

ent)

The

algo

rithm

s in

FR

EALI

GN

hav

e ef

ficie

nt p

roce

dure

s fo

r re

finin

g 3D

stru

ctur

es b

y w

orki

ng e

ntire

ly in

Fou

rier s

pace

.

N. G

rigor

ieff

/ Jou

rnal

of S

truct

ural

Bio

logy

157

(200

7) 1

17–1

25

3d m

odel

2d

pro

j Im

ages

st

ack

FT o

f pro

j FT

of I

m

Mat

chin

g pr

oced

ure

CTF

re

finem

ent

New

3D

3D F

T FT

-1

EM m

grs

Rec

omm

enda

tions

1.D

on’t

star

t fro

m a

sym

met

rical

vie

w.

2.Tr

y to

sta

rt fro

m th

e ge

nera

l (co

mm

on) v

iew,

then

the

seco

nd c

an b

e sy

mm

etric

al.

3.Tr

y to

use

as

man

y D

IFFE

REN

T vi

ews

as p

ossi

ble,

idea

lly

perp

endi

cula

r to

each

oth

er.

4.D

o no

t use

a s

eque

nce

of s

imila

r vie

ws,

the

prog

ram

will

be c

onfu

sed!

5.

If th

e st

anda

rd d

evia

tion

of p

eak

heig

hts

star

ts to

incr

ease

, it

mea

ns th

at th

e pr

oces

s is

sta

rting

to d

iver

ge.

You

will

not g

et a

reas

onab

le s

olut

ion.

6.

Che

ck th

e an

gula

r dis

tribu

tion

of p

roje

ctio

ns

Page 13: Images of molecules in vitreous ice - …embo2017.cryst.bbk.ac.uk/embo2017/course/Lectures/Lecture 11... · Common lines in real space The angular reconstitution method is based on

Met

hods

of o

rient

atio

n de

term

inat

ion:

1.

Con

ical

tilt.

It is

mor

e ef

ficie

nt fo

r neg

ativ

ely

stai

ned

sam

ples

with

a p

refe

rabl

e or

ient

atio

n.

M

isse

d co

ne

Le

schz

iner

AE,

Nog

ales

E. T

he o

rtho

gona

l tilt

reco

nstr

uctio

n m

etho

d:

an a

ppro

ach

to g

ener

atin

g si

ngle

-cla

ss v

olum

es w

ith n

o m

issi

ng c

one

for a

b in

itio

reco

nstr

uctio

n of

asy

mm

etric

par

ticle

s. J

Str

uct B

iol.

2006

M

ar;1

53(3

):284

-99

2. A

ngul

ar re

cons

titut

ion.

It re

quire

s go

od s

igna

l/noi

se

ratio

, nee

ds c

lass

ifica

tion

3. C

omm

on li

nes

in F

ourie

r spa

ce a

nd P

FT a

re m

ostly

us

ed a

t ana

lysi

s of

par

ticle

s w

ith ic

osah

edra

l sy

mm

etry

4.

Pro

ject

ion

mat

chin

g, th

e m

ost p

opul

ar te

chni

que,

requ

ires

an in

itial

mod

el.

5. F

REA

LIG

N -

impl

emen

ted

in R

elio

n, F

ourie

r spe

ctra

m

atch

ing,

nee

ds a

n in

itial

mod

el

Ref

eren

ces:

1.R

adon

, J. (

1917

) Ube

r di

e B

estim

mun

g vo

n Fu

nktio

nen

durc

h ih

re In

tegr

alw

erte

ngs g

ewis

ser

Man

nigf

altig

keite

n. B

er. S

achs

. Aka

d. W

iss.

Leip

zig.

Kl.,

69,

110

7-11

14

2.C

row

ther

, .A

., D

eRos

ier,

D.J.

, and

Klu

g,A

. (19

70) T

he r

econ

stru

ctio

n of

a th

ree-

dim

ensi

onal

stru

ctur

e fr

om p

roje

ctio

ns a

nd it

s app

licat

ion

to e

lect

ron

mic

rosc

opy.

Pr

oc. R

.Soc

. Lon

d, 3

17, 3

19-3

40

3.Va

n H

eel,

M. (

1987

) Ang

ular

rec

onst

itutio

n: a

pos

teri

ori a

ssig

nmen

t of p

roje

ctio

n di

rect

ions

for

3D r

econ

stru

ctio

ns. U

ltram

icro

scop

y, 21

, 114

-126

4.

Sery

shev

a, I.

, Orlo

va, E

.V.,

Sher

man

, M.,

Chi

u, W

., H

amilt

on, S

., a

nd v

an H

eel,

M.,

(199

5) T

he sk

elet

al m

uscl

e ca

lciu

m-r

elea

se c

hann

el in

its c

lose

d st

ate

visu

aliz

ed b

y el

ectr

on m

icro

scop

y an

d an

gula

r re

cons

titut

ion.

Nat

ure

Stru

ct. B

iol.

, 2, 1

8-14

5.

Rad

erm

ache

r, M

. (19

88) T

he th

ree-

dim

ensi

onal

rec

onst

ruct

ion

of si

ngle

par

ticle

s fo

rm r

ando

m a

nd n

on-r

ando

m ti

lt se

ries

. J. E

lect

ron

Mic

rosc

. Tec

h. 9

, 359

-394

6.

Penc

zek,

P.,

Gra

ssuc

i, R

.A.,

and

Fran

k, J.

(199

4) T

he r

ibos

ome

at im

prov

ed

reso

lutio

n: N

ew te

chni

ques

for

mer

ging

and

ori

enta

tion

refin

emen

t in

3D

cryo

elec

tron

mic

rosc

opy

of b

iolo

gica

l par

ticle

s. U

ltram

icro

scop

y, 53

, 251

-270

7.

Fulle

r SD

, But

cher

SJ,

Che

ng R

H, B

aker

TS

(199

6) T

hree

-dim

ensi

onal

re

cons

truc

tion

of ic

osah

edra

l par

ticle

s--t

he u

ncom

mon

line

. J S

truc

t Bio

l. 11

6, 4

8-55

.

Ref

eren

ces

Grig

orie

ff, N

. 20

07.

FREA

LIG

N: h

igh-

reso

lutio

n re

finem

ent o

f sin

gle

parti

cle

stru

ctur

es. J

Stru

ct B

iol.

157:

117–

125.

Si

ndel

ar, C

V, G

rigor

ieff

N.

2012

. O

ptim

al n

oise

redu

ctio

n in

3D

re

cons

truct

ions

of s

ingl

e pa

rticl

es u

sing

a v

olum

e-no

rmal

ized

filte

r. J

Stru

ct

Biol

. 180

:26-

38.

Lyum

kis,

D, B

rilot

AF,

The

obal

d D

L, G

rigor

ieff

N.

2013

. Li

kelih

ood-

base

d cl

assi

ficat

ion

of c

ryo-

EM im

ages

usi

ng F

REA

LIG

N. J

Stru

ct B

iol.

183:

377-

388.