RIP and RIPAS phasing with the help of SHELXC/D/E

Transcription

RIP and RIPAS phasing with the help of SHELXC/D/E
Radiation Damage Induced Phasing
Max Nanao
ACA 2016
RADIATION DAMAGE INDUCED PHASING REVIEW
X-rays induce changes to macromolecular crystals via radiation damage
Global changes/damage
Molecular rotations
Unit cell changes
Specific changes/damage
Lowered occupancy of heavy atoms (Se, Br, Hg…)
Breakage of S-S bonds
Decarboxylation
Dehydroxylation
RNAse, +/- 8 σ
Trypsin, +/- 8 σ
SPECIFIC DAMAGE CAN BE USED TO PHASE MACROMOLECULES: PHASES FOR
FREE!
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RIP PHASING PREMISE
+
Hg
Hg
SIR
RIP
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l Title of Presentation l Date of Presentation l Author
SYNCHROTRON RIP – A ONE MINUTE REVIEW
Specific radiation damage used in an “inverted SIR” experiment
Specific damage àSignal
Disulfides, metals, carboxylates
General damageàNoise
Which is the native?
Un-damaged = “Derivative” aka “Before damage”
Damaged = “Native” aka “After damage”
Substructure and phases can be determined experimentally
août 1,
2016
5
SOME RIP POSITIVES
No modification of the protein necessary
Works for disulfides and/or HAs (ok, a little
modification)
Can be performed on a fixed energy
beamlines
High degree of isomorphism if dose is
managed (same xtal, same position)
RIP PHASING SCHEME
“burn”
“after”
“before”
Calculate
Differences, and
statistics (SHELXC)
Determine structure of
damage (SHELXD)
Calculate phases of whole
protein, build model
(SHELXE)
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7
RIP ISSUES AND DIFFICULTIES
Radiation damage
substructures are more
complex
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
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RIP ISSUES AND DIFFICULTIES
Radiation damage
substructures are more
complex
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
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9
RIP substructure can be improved
iteratively by difference Fourier
based substructure revision:
“recycling” (SHELXE)
RIP ISSUES AND DIFFICULTIES
Radiation damage
substructures are more
complex
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
01/08/16
10
RIP substructure can be improved
iteratively by difference Fourier
based substructure revision:
“recycling” (SHELXE)
RIP ISSUES AND DIFFICULTIES
Radiation damage
substructures are more
complex
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
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Early RIP maps revealed
many small negative peaks in
unexpected places à Fafter
overscaled!
RIP ISSUES AND DIFFICULTIES
Radiation damage
substructures are more
complex
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
01/08/16
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Early RIP maps revealed
many small negative peaks in
unexpected places à Fafter
overscaled!
overscaled!à
Many substructures not
solvable!
RIP ISSUES AND DIFFICULTIES
Radiation damage
substructures are more
complex
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
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For substructure
determination: down scale
“After” dataset by K
For Phasing: scale can be
refined (e.g. in SHARP)
RIP ISSUES AND DIFFICULTIES
No downscaling
Radiation damage
substructures are more
complex
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
SHELXD
CC
K
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RIP ISSUES AND DIFFICULTIES
Radiation damage
substructures are more
complex
Phase error vs. scale
Large
Negatively occupied sites
Scaling between before
and after datasets can be
difficult
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RIP substructure can be improved
by adjusting the before/after scale
(SHELXC DSCA)
IMPORTANT SHELX KEYWORDS FOR RIP
SHELXC
RIP
RIPA
DSUL
DSCA
SHELXE
-b Revised heavy atom sites
-h Heavy atoms in native
(-z) still untested
(-a) may reduce need for recycling?
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THE MANY FACES OF RIP
Classic RIP
A-burn-B
Classic UV RIP
A-UV-B (Laser or LED)
Segmented RIP
Classic RIP
Classic UV RIP
Segmented RIP
Serial X-ray RIP
Collect large dataset, split up into sub
datasets
Serial X-ray RIP
Serial UV-RIP
Collect sub datasets from many crystals
High intensity RIP
Serial UV-RIP
Collect sub datasets from many crystals
High intensity RIP
At high fluence (i.e. XFEL) , heavier atom
occupancy preferentially reduced
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THE MANY FACES OF RIP
Classic RIP
A-burn-B
+Easy
-Difficult to estimate
burn dose
-Diffractive life of
crystal is wasted
Classic UV RIP
A-UV-B (Laser or LED)
Segmented RIP
Collect large dataset, split up into sub
datasets
Serial X-ray RIP
Collect sub datasets from many crystals
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Burn: With accurate estimates of
absorbed dose (calibrated diodes,
RADDOSE) and/or online
microspectrophotometers, this
process can be simplified
THE MANY FACES OF RIP
Classic RIP
A-burn-B
Classic UV RIP
A-UV-B (Laser or LED)
+Improved signal
Less noise from
global damage
-Fewer groups affected (no
carboxylates)
Different wavelength of laser?
-Difficult to estimate UV
burn
Interleave X-ray datasets with UV burns
-Penetration depth is small
Smaller xtals (see serial approach)
-Alignment of light source
can be difficult
UVLEDs
Acta Crystallogr D Struct Biol. 2016 Mar;72(Pt 3):395-402.
Radiation-damage-induced phasing: a case study using UV irradiation with light-emitting diodes.
de Sanctis D, Zubieta C, Felisaz F, Caserotto H, Nanao MH.
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THE MANY FACES OF RIP
Classic RIP
A-burn-B
Large oscillation dataset
Classic UV RIP
A-UV-B (Laser or LED)
“before” dataset
“after” dataset
Segmented RIP
Collect large dataset, split up
into sub datasets
+No burn
+Signal:Noise can be
optimised computationally
+Diffractive life not wasted
-Computationally intensive
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RIP
THE MANY FACES OF RIP
Classic RIP
A-burn-B
Classic UV RIP
A-UV-B (Laser or LED)
Segmented RIP
Collect large dataset, split up into sub datasets
Serial X-ray RIP
Collect sub datasets from many crystals
+Dose multiplier!
+Extend useful range of crystal
by RIP (needed single xtals
big enough for multiple
datasets before)
-Non isomorphism, merging
difficult
-Long collection times
(diffractive map,
sub-dataset collection)
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MeshAndCollect: an automated multi-crystal data-collection workflow for
synchrotron macromolecular crystallography beamlines.
Zander U, Bourenkov G, Popov AN, de Sanctis D, Svensson O,
McCarthy AA, Round E, Gordeliy V, Mueller-Dieckmann C, Leonard GA.
Acta Crystallogr D Biol Crystallogr. 2015 Nov;71(Pt 11):2328-43
Repeat until specific
damage is accumulated
(normally at 2 MGy)
THE MANY FACES OF RIP
Classic RIP
A-burn-B
Classic UV RIP
A-UV-B (Laser or LED)
Segmented RIP
Collect large dataset, split up into sub datasets
Serial X-ray RIP
Collect sub datasets from many crystals
Serial UV-RIP
Collect sub datasets from many crystals
High intensity RIP
At high fluence (i.e. XFEL) , heavier
atom occupancy preferentially reduced
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“before”/low
fluence
“after”/high
fluence
Towards RIP using free-electron laser SFX data.
Galli L, Son SK, White TA, Santra R, Chapman HN, Nanao MH.
J Synchrotron Radiat. 2015
Multiwavelength anomalous diffraction at high x-ray intensity.
Son SK, Chapman HN, Santra R.
Phys Rev Lett. 2015
Towards phasing using high X-ray intensity.
Galli L, Son SK, Barends TR, White TA, Barty A, Botha S, Boutet S, Caleman C, Doak RB, Nanao MH, Nass K,
Shoeman RL, Timneanu N, Santra R, Schlichting I, Chapman HN.
IUCrJ. 2015
THE MANY FACES OF RIP
Classic RIP
A-burn-B
Classic UV RIP
A-UV-B (Laser or LED)
Segmented RIP
Collect large dataset, split up into sub datasets
Serial X-ray RIP
Collect sub datasets from many crystals
Serial UV-RIP
Collect sub datasets from many crystals
High intensity RIP
At high fluence (i.e. XFEL) , heavier
atom occupancy preferentially reduced
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Towards RIP using free-electron laser SFX data.
Galli L, Son SK, White TA, Santra R, Chapman HN, Nanao MH.
J Synchrotron Radiat. 2015
Multiwavelength anomalous diffraction at high x-ray intensity.
Son SK, Chapman HN, Santra R.
Phys Rev Lett. 2015
Towards phasing using high X-ray intensity.
Galli L, Son SK, Barends TR, White TA, Barty A, Botha S, Boutet S, Caleman C, Doak RB, Nanao MH, Nass K,
Shoeman RL, Timneanu N, Santra R, Schlichting I, Chapman HN.
IUCrJ. 2015
CONCLUSIONS
Comclusions
Specific radiation damage can be used in various types of MX
experiments to determine phases de novo
RIP is similar but not identical to SIR and requires that we take specific
measures
SHELX has been specifically modified to work with RIP
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l Title of Presentation l Date of Presentation l Author
THE MANY FACES OF RIP
ACKNOWLEDGEMENTS
Classic RIP
A-burn-B
Daniele de Sanctis
Raimond Ravelli
Classic UV RIP
A-UV-B (Laser or LED)
George Sheldrick
Segmented RIP
Elspeth Garman
Collect large dataset, split up into sub datasets
Andrew McCarthy
Serial X-ray RIP
Lorenzo Galli
Collect sub datasets from many crystals
Serial UV-RIP
Sang-Kil Son
Collect sub datasets from many crystals
HenryRIP
Chapman
High intensity
Nicolas
Foos
At high
fluence (i.e.
XFEL) , heavier
atom occupancy preferentially reduced
+Novel phasing method for
FELs
-Still theoretical
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