Difference between revisions of "User Stories:BETA-BLIP"

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The case of β-lactamase (BETA)–β-
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The case of β-lactamase (BETA)–β-lactamase inhibitor (BLIP) has been used repeatedly as a test case for Phaser because the original structure solution by MR using AMoRe (Navaza, 1994) was difficult even though good models were available (the structures of both components had already been solved in isolation; Strynadka et al., 1996). The difficult part of the MR solution was placing BLIP. The command script for the solution of BETA–BLIP using the ‘automated MR’ mode of Phaser is shown in Appendix A1. The search order is given as BETA and then BLIP. This is because BETA, with 62% of the molecular weight, would be expected to have the highest fraction scattering (and indeed it does, as the B factors for BETA and BLIP are comparable). Phaser rapidly produces a correct solution for the complex.  
lactamase inhibitor (BLIP) has been
+
 
used repeatedly as a test case for Phaser
+
This previously difficult structure solution becomes trivial because of two algorithms implemented in Phaser. *The first is the anisotropy correction; there is significant anisotropy in the data (the maximum B-factor difference in different directions is 32 Ų).  
(Storoni et al., 2004; McCoy et al., 2005)
+
*The second is the improved rotation-function target in MLRF, particularly in that the solution for BETA can be used to find the correct rotation-function solution for BLIP. Using the traditional Crowther (1972) fast rotation function, the Z score for the correct BLIP placement is 3.8 and the top Z score of 4.4 corresponds to an incorrect placement. Using MLRF and the prior knowledge about the placement of BETA, the correct placement of BLIP has a Z score of 6.5 and is the highest score in the search. (These results are for data that have had the anisotropy correction applied, to illustrate the improvement given by the MLRF alone.)
because the original structure solution
 
by MR using AMoRe (Navaza, 1994)
 
was difficult even though good models
 
were available (the structures of both
 
components had already been solved in
 
isolation; Strynadka et al., 1996; Fig. 4a).
 
The difficult part of the MR solution
 
was placing BLIP.
 
The command script for the solution
 
of BETA–BLIP using the ‘automated
 
MR’ mode of Phaser is shown in
 
Appendix A1. The search order is given as BETA and then
 
BLIP. This is because BETA, with 62% of the molecular
 
weight, would be expected to have the highest fraction scattering
 
(and indeed it does, as the B factors for BETA and
 
BLIP are comparable). Phaser rapidly produces a correct
 
solution for the complex. This previously difficult structure
 
solution becomes trivial because of two algorithms implemented
 
in Phaser. The first is the anisotropy correction; there
 
is significant anisotropy in the data (the maximum B-factor
 
difference in different directions is 32 A ° 2). The second is the
 
improved rotation-function target in MLRF, particularly in
 
that the solution for BETA can be used to find the correct
 
rotation-function solution for BLIP. Using the traditional
 
Crowther (1972) fast rotation function, the Z score for the
 
correct BLIP placement is 3.8 and the top Z score of 4.4
 
corresponds to an incorrect placement. Using MLRF and the
 
prior knowledge about the placement of BETA, the correct
 
placement of BLIP has a Z score of 6.5 and is the highest score
 
in the search. (These results are for data that have had the
 
anisotropy correction applied, to illustrate the improvement
 
given by the MLRF alone.)
 

Revision as of 21:20, 11 July 2009

Crystallographic details
Space Group P3221
Unit Cell
Contents of
asymmetric unit
BETA and BLIP
Models 100% identity

The case of β-lactamase (BETA)–β-lactamase inhibitor (BLIP) has been used repeatedly as a test case for Phaser because the original structure solution by MR using AMoRe (Navaza, 1994) was difficult even though good models were available (the structures of both components had already been solved in isolation; Strynadka et al., 1996). The difficult part of the MR solution was placing BLIP. The command script for the solution of BETA–BLIP using the ‘automated MR’ mode of Phaser is shown in Appendix A1. The search order is given as BETA and then BLIP. This is because BETA, with 62% of the molecular weight, would be expected to have the highest fraction scattering (and indeed it does, as the B factors for BETA and BLIP are comparable). Phaser rapidly produces a correct solution for the complex.

This previously difficult structure solution becomes trivial because of two algorithms implemented in Phaser. *The first is the anisotropy correction; there is significant anisotropy in the data (the maximum B-factor difference in different directions is 32 Ų).

  • The second is the improved rotation-function target in MLRF, particularly in that the solution for BETA can be used to find the correct rotation-function solution for BLIP. Using the traditional Crowther (1972) fast rotation function, the Z score for the correct BLIP placement is 3.8 and the top Z score of 4.4 corresponds to an incorrect placement. Using MLRF and the prior knowledge about the placement of BETA, the correct placement of BLIP has a Z score of 6.5 and is the highest score in the search. (These results are for data that have had the anisotropy correction applied, to illustrate the improvement given by the MLRF alone.)