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Re: [ccp4bb] tricky molecular replacement |
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CCP4bb navigationCCP4bb <-- 1999 <-- November 1999 <-- 30 November 1999Subject: Re: tricky molecular replacement From: "Randy J {- dot -} Read" rjr27 {- at -} CAM {- dot -} AC {- dot -} UK Date: 2007-11-03 If you take a PDB file from the solution for the hexagonal form as your input model for a translation search in P1, then the cross-rotation peaks that rotate the hexagonal data onto the P1 data should be the correct orientations. (Phaser uses the same definition for Euler angles as ALMN.) I'd give a generous list of orientations, because the translation searches are very fast. These should include symmetry equivalent cross-rotation peaks, because there's only one copy of the model and you don't know which symmetry-related orientation to apply to that one. What you would like to see (apart from a clear solution!) is that the two orientations are related by the same rotation that you see in the P1 self-rotation function. Randy Read On Nov 3 2007, Jan Abendroth wrote: >Hi all, >I have a tricky molecular replacement case. One protein in two different >crystal forms: hexagonal with 1 mol/asu, triclinic with 2 mol/asu (based on >packing and self rotation). > > No experimental phases are available this far, however, there is a > distant homology model. For the hexagonal crystals, phaser gives a > solution with really good scores (Z > 9, -LLG > 50) and a good packing. > While the correct solution is way down the list in the RF, the TF can > separate it from the bulk of bad solutions. Slight changes in the model > give the same solution. Maps are somehow ok, however, not good enough to > enable arpwarp to build the model. It does not totally blow up either. > >For the triclinic crystal form with 2 molecules related by a two-fold which >is not parallel to a crystal axis, phaser does not find a solution. Neither >does molrep using the locked rotation function with the two-fold extracted >by the SRF. > > As the homology between the data set should be higher than between the > model in the data sets and the search model, I tried a cross rotation > function between the two data sets. Strong peaks there should give the > relation between the orientation of the molecule in the hexagonal crystal > (that I believe I can find). With two rotations known and one translation > undefined, I'd be left with only one translation that needs to be found. > Then averaging within P1 or cross crystal might improve the density... > > Almn appears to be the only program in ccp4 that can do a cross rotation > using Fs only, right?? I used the P1 data as hklin, the hexagonal data as > hklin2. Almn comes back with two strong peaks (see below), however, now I > am lost: - the first two peaks appear to be the same - are the Euler > angles the ones I could use in a peak list for eg. Phaser? - does this > procedure make sense at all? - any other ideas? > >Thanks a lot >Jan > >almn.log: >########## > Peaks must be greater than 2.00 times RMS density 52.2161 > > > > Eulerian angles Polar angles > > Alpha Beta Gamma Peak Omega Phi >Kappa Direction cosines >PkNo Symm: 1 2 > > Peak 1 > 1 1 1 323.7 143.4 18.5 540.8 92.9 62.6 >143.8 0.4594 0.8867 -0.0511 > 1 1 2 323.7 143.4 78.5 540.8 83.2 32.6 >145.9 0.8364 0.5351 0.1184 > 1 1 3 323.7 143.4 138.5 540.8 75.6 2.6 >157.2 0.9674 0.0441 0.2495 > 1 1 4 323.7 143.4 198.5 540.8 71.9 332.6 >174.4 0.8439 -0.4373 0.3108 > 1 1 5 323.7 143.4 258.5 540.8 107.2 122.6 >167.0 -0.5149 0.8049 -0.2950 > 1 1 6 323.7 143.4 318.5 540.8 101.7 92.6 >151.7 -0.0446 0.9781 -0.2034 > 1 1 7 143.7 36.6 41.5 540.8 161.7 321.1 >175.0 0.2448 -0.1974 -0.9493 > 1 1 8 143.7 36.6 341.5 540.8 20.4 171.1 >128.2 -0.3451 0.0540 0.9370 > 1 1 9 143.7 36.6 281.5 540.8 31.6 201.1 >73.8 -0.4882 -0.1885 0.8521 > 1 1 10 143.7 36.6 221.5 540.8 82.2 231.1 >37.0 -0.6220 -0.7711 0.1363 > 1 1 11 143.7 36.6 161.5 540.8 144.3 261.1 >65.1 -0.0902 -0.5770 -0.8118 > 1 1 12 143.7 36.6 101.5 540.8 158.6 291.1 >118.5 0.1317 -0.3411 -0.9307 > > Peak 2 > 2 1 1 143.7 36.6 41.5 540.8 161.7 321.1 >175.0 0.2448 -0.1974 -0.9493 > 2 1 2 143.7 36.6 101.5 540.8 158.6 291.1 >118.5 0.1317 -0.3411 -0.9307 > 2 1 3 143.7 36.6 161.5 540.8 144.3 261.1 >65.1 -0.0902 -0.5770 -0.8118 > 2 1 4 143.7 36.6 221.5 540.8 82.2 231.1 >37.0 -0.6220 -0.7711 0.1363 > 2 1 5 143.7 36.6 281.5 540.8 31.6 201.1 >73.8 -0.4882 -0.1885 0.8521 > 2 1 6 143.7 36.6 341.5 540.8 20.4 171.1 >128.2 -0.3451 0.0540 0.9370 > 2 1 7 323.7 143.4 18.5 540.8 92.9 62.6 >143.8 0.4594 0.8867 -0.0511 > 2 1 8 323.7 143.4 318.5 540.8 101.7 92.6 >151.7 -0.0446 0.9781 -0.2034 > 2 1 9 323.7 143.4 258.5 540.8 107.2 122.6 >167.0 -0.5149 0.8049 -0.2950 > 2 1 10 323.7 143.4 198.5 540.8 71.9 332.6 >174.4 0.8439 -0.4373 0.3108 > 2 1 11 323.7 143.4 138.5 540.8 75.6 2.6 >157.2 0.9674 0.0441 0.2495 > 2 1 12 323.7 143.4 78.5 540.8 83.2 32.6 >145.9 0.8364 0.5351 0.1184 > > Peak 3 > 3 1 1 335.2 54.5 36.5 209.2 78.8 59.3 >55.6 0.5006 0.8437 0.1940 ... > Peak 4 > 4 1 1 155.2 125.5 23.5 209.2 62.8 155.8 >179.4 -0.8112 0.3638 0.4579 ... > Peak 5 > 5 1 1 349.3 53.8 13.0 176.4 87.7 78.2 >53.9 0.2051 0.9779 0.0406 ... > CCP4bb navigationCCP4bb <-- 1999 <-- November 1999 <-- 30 November 1999 |
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