examples/1I2T.tar.bz2
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Binary files /dev/null and b/examples/1I2T.tar.bz2 differ
examples/phenix.rosetta_refine.log
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+
2
+============================== Collecting inputs ==============================
3
+
4
+
5
+ ----------Processing X-ray data----------
6
+
7
+I-obs:
8
+ /nfs/staff/key/software_tests/PHENIX.ROSETTA.REFINE_linux/1I2T_F.mtz:IOBS,SIGIOBS
9
+Miller array info: /nfs/staff/key/software_tests/PHENIX.ROSETTA.REFINE_linux/1I2T_F.mtz:IOBS,SIGIOBS
10
+Observation type: xray.intensity
11
+Type of data: double, size=31449
12
+Type of sigmas: double, size=31449
13
+Number of Miller indices: 31449
14
+Anomalous flag: False
15
+Unit cell: (32.969, 38.166, 51.062, 90, 90, 90)
16
+Space group: P 21 21 21 (No. 19)
17
+Systematic absences: 0
18
+Centric reflections: 3439
19
+Resolution range: 19.083 1.04105
20
+Completeness in resolution range: 0.996609
21
+Completeness with d_max=infinity: 0.996388
22
+Wavelength: 1.1000
23
+
24
+
25
+ ----------Scaling input intensities via French-Wilson Method----------
26
+
27
+Trying 60 bins...
28
+Number of bins = 60
29
+** Calculating bin mean intensity values for each intensity **
30
+** Total # rejected intensities: 0 **
31
+Intensities converted to amplitudes for use in refinement.
32
+
33
+Number of F-obs in resolution range: 31449
34
+Number of F-obs<0 (these reflections will be rejected): 0
35
+Number of F-obs=0 (these reflections will be used in refinement): 0
36
+Refinement resolution range: d_max = 19.0830
37
+ d_min = 1.0411
38
+
39
+R-free flags:
40
+ /nfs/staff/key/software_tests/PHENIX.ROSETTA.REFINE_linux/1I2T_F.mtz:FreeR_flag
41
+Miller array info: /nfs/staff/key/software_tests/PHENIX.ROSETTA.REFINE_linux/1I2T_F.mtz:FreeR_flag
42
+Observation type: None
43
+Type of data: int, size=31567
44
+Type of sigmas: None
45
+Number of Miller indices: 31567
46
+Anomalous flag: False
47
+Unit cell: (32.969, 38.166, 51.062, 90, 90, 90)
48
+Space group: P 21 21 21 (No. 19)
49
+Systematic absences: 0
50
+Centric reflections: 3486
51
+Resolution range: 30.5703 1.041
52
+Completeness in resolution range: 1
53
+Completeness with d_max=infinity: 1
54
+Wavelength: 9.9990
55
+
56
+Test (R-free flags) flag value: 0
57
+
58
+Number of work/free reflections by resolution:
59
+ work free %free
60
+ bin 1: 19.0862 - 2.2418 [3340/3340] 3188 152 4.6%
61
+ bin 2: 2.2418 - 1.7798 [3216/3217] 3050 166 5.2%
62
+ bin 3: 1.7798 - 1.5549 [3147/3150] 2995 152 4.8%
63
+ bin 4: 1.5549 - 1.4128 [3136/3137] 2983 153 4.9%
64
+ bin 5: 1.4128 - 1.3116 [3144/3146] 2979 165 5.2%
65
+ bin 6: 1.3116 - 1.2343 [3134/3134] 2981 153 4.9%
66
+ bin 7: 1.2343 - 1.1725 [3107/3107] 2951 156 5.0%
67
+ bin 8: 1.1725 - 1.1214 [3108/3114] 2950 158 5.1%
68
+ bin 9: 1.1214 - 1.0783 [3103/3128] 2951 152 4.9%
69
+ bin 10: 1.0783 - 1.0411 [3014/3083] 2860 154 5.1%
70
+ overall 29888 1561 5.0%
71
+
72
+ ----------Processing PDB file(s)----------
73
+
74
+ Monomer Library directory:
75
+ "/programs/x86_64-linux/phenix/1.13-2998/phenix-1.13-2998/modules/chem_data/mon_lib"
76
+ Total number of atoms: 602
77
+ Number of models: 1
78
+ Model: ""
79
+ Number of chains: 2
80
+ Chain: "A"
81
+ Number of atoms: 472
82
+ Number of conformers: 1
83
+ Conformer: ""
84
+ Number of residues, atoms: 61, 472
85
+ Classifications: {'peptide': 61}
86
+ Modifications used: {'COO': 1}
87
+ Link IDs: {'PTRANS': 3, 'TRANS': 57}
88
+ Chain: "A"
89
+ Number of atoms: 130
90
+ Number of conformers: 1
91
+ Conformer: ""
92
+ Number of residues, atoms: 130, 130
93
+ Classifications: {'water': 130}
94
+ Link IDs: {None: 129}
95
+ Time building chain proxies: 0.35, per 1000 atoms: 0.58
96
+ Number of scatterers: 602
97
+ At special positions: 0
98
+ Unit cell: (32.969, 38.166, 51.062, 90, 90, 90)
99
+ Space group: P 21 21 21 (No. 19)
100
+ Number of sites at special positions: 0
101
+ Number of scattering types: 4
102
+ Type Number sf(0)
103
+ S 3 16.00
104
+ O 216 8.00
105
+ N 85 7.00
106
+ C 298 6.00
107
+ sf(0) = scattering factor at diffraction angle 0.
108
+
109
+ Number of disulfides: simple=0, symmetry=0
110
+ Custom bonds:
111
+ Warning: Ignoring bond with distance_ideal = None:
112
+ atom_selection_1 = None
113
+ atom_selection_2 = None
114
+ Total number of custom bonds: 0
115
+ Custom angles:
116
+ Warning: Ignoring angle with angle_ideal = None:
117
+ atom_selection_1 = None
118
+ atom_selection_2 = None
119
+ atom_selection_3 = None
120
+ Total number of custom angles: 0
121
+ Custom dihedrals:
122
+ Warning: Ignoring dihedral with angle_ideal = None:
123
+ atom_selection_1 = None
124
+ atom_selection_2 = None
125
+ atom_selection_3 = None
126
+ atom_selection_4 = None
127
+ Total number of custom dihedrals: 0
128
+ Custom planarities:
129
+ Warning: Ignoring planarity with with sigma <= 0:
130
+ atom_selection = None
131
+None
132
+ Total number of custom planarities: 0
133
+ Custom parallelities:
134
+Warning: Ignoring parallelity with empty atom selection.
135
+ Total number of custom parallelities: 0
136
+
137
+ Automatic linking
138
+ Parameters for automatic linking
139
+ Linking & cutoffs
140
+ Metal : False - 3.50
141
+ Amimo acid : False - 1.90
142
+ Carbohydrate : True - 1.99
143
+ Ligands : True - 1.99
144
+ Small molecules : False - 1.98
145
+ Amino acid - RNA/DNA : False
146
+
147
+ Number of custom bonds: simple=0, symmetry=0
148
+ Time building additional restraints: 0.11
149
+ Conformation dependent library (CDL) restraints added in 24.1 milliseconds
150
+
151
+ Adding C-beta torsion restraints...
152
+ Number of C-beta restraints generated: 116
153
+
154
+ Time building geometry restraints manager: 0.14 seconds
155
+
156
+ NOTE: a complete listing of the restraints can be obtained by requesting
157
+ output of .geo file.
158
+
159
+ Histogram of bond lengths:
160
+ 1.22 - 1.35: 161
161
+ 1.35 - 1.48: 94
162
+ 1.48 - 1.61: 217
163
+ 1.61 - 1.74: 0
164
+ 1.74 - 1.87: 6
165
+ Bond restraints: 478
166
+ Sorted by residual:
167
+ bond pdb=" C GLY A1069 "
168
+ pdb=" OXT GLY A1069 "
169
+ ideal model delta sigma weight residual
170
+ 1.231 1.363 -0.132 2.00e-02 2.50e+03 4.36e+01
171
+ bond pdb=" CG MET A1024 "
172
+ pdb=" SD MET A1024 "
173
+ ideal model delta sigma weight residual
174
+ 1.803 1.874 -0.071 2.50e-02 1.60e+03 8.11e+00
175
+ bond pdb=" CG MET A1035 "
176
+ pdb=" SD MET A1035 "
177
+ ideal model delta sigma weight residual
178
+ 1.803 1.873 -0.070 2.50e-02 1.60e+03 7.94e+00
179
+ bond pdb=" SD MET A1035 "
180
+ pdb=" CE MET A1035 "
181
+ ideal model delta sigma weight residual
182
+ 1.791 1.849 -0.058 2.50e-02 1.60e+03 5.41e+00
183
+ bond pdb=" SD MET A1024 "
184
+ pdb=" CE MET A1024 "
185
+ ideal model delta sigma weight residual
186
+ 1.791 1.842 -0.051 2.50e-02 1.60e+03 4.10e+00
187
+ ... (remaining 473 not shown)
188
+
189
+ Histogram of bond angle deviations from ideal:
190
+ 96.82 - 105.53: 15
191
+ 105.53 - 114.23: 281
192
+ 114.23 - 122.94: 314
193
+ 122.94 - 131.65: 32
194
+ 131.65 - 140.35: 3
195
+ Bond angle restraints: 645
196
+ Sorted by residual:
197
+ angle pdb=" CA GLY A1069 "
198
+ pdb=" C GLY A1069 "
199
+ pdb=" OXT GLY A1069 "
200
+ ideal model delta sigma weight residual
201
+ 121.00 140.35 -19.35 3.00e+00 1.11e-01 4.16e+01
202
+ angle pdb=" O GLY A1069 "
203
+ pdb=" C GLY A1069 "
204
+ pdb=" OXT GLY A1069 "
205
+ ideal model delta sigma weight residual
206
+ 118.00 99.51 18.49 3.00e+00 1.11e-01 3.80e+01
207
+ angle pdb=" CA HIS A1068 "
208
+ pdb=" CB HIS A1068 "
209
+ pdb=" CG HIS A1068 "
210
+ ideal model delta sigma weight residual
211
+ 113.80 118.12 -4.32 1.00e+00 1.00e+00 1.86e+01
212
+ angle pdb=" CB GLN A1011 "
213
+ pdb=" CG GLN A1011 "
214
+ pdb=" CD GLN A1011 "
215
+ ideal model delta sigma weight residual
216
+ 112.60 119.69 -7.09 1.70e+00 3.46e-01 1.74e+01
217
+ angle pdb=" OE1 GLN A1011 "
218
+ pdb=" CD GLN A1011 "
219
+ pdb=" NE2 GLN A1011 "
220
+ ideal model delta sigma weight residual
221
+ 122.60 119.13 3.47 1.00e+00 1.00e+00 1.21e+01
222
+ ... (remaining 640 not shown)
223
+
224
+ Histogram of dihedral angle deviations from ideal:
225
+ 0.01 - 16.59: 280
226
+ 16.59 - 33.16: 16
227
+ 33.16 - 49.74: 3
228
+ 49.74 - 66.32: 1
229
+ 66.32 - 82.89: 1
230
+ Dihedral angle restraints: 301
231
+ sinusoidal: 124
232
+ harmonic: 177
233
+ Sorted by residual:
234
+ dihedral pdb=" CB MET A1062 "
235
+ pdb=" CG MET A1062 "
236
+ pdb=" SD MET A1062 "
237
+ pdb=" CE MET A1062 "
238
+ ideal model delta sinusoidal sigma weight residual
239
+ -60.00 -108.96 48.96 3 1.50e+01 4.44e-03 8.71e+00
240
+ dihedral pdb=" CA PHE A1028 "
241
+ pdb=" C PHE A1028 "
242
+ pdb=" N ALA A1029 "
243
+ pdb=" CA ALA A1029 "
244
+ ideal model delta harmonic sigma weight residual
245
+ -180.00 -167.77 -12.23 0 5.00e+00 4.00e-02 5.98e+00
246
+ dihedral pdb=" CB GLN A1011 "
247
+ pdb=" CG GLN A1011 "
248
+ pdb=" CD GLN A1011 "
249
+ pdb=" OE1 GLN A1011 "
250
+ ideal model delta sinusoidal sigma weight residual
251
+ 180.00 97.11 82.89 2 3.00e+01 1.11e-03 5.25e+00
252
+ ... (remaining 298 not shown)
253
+
254
+ Histogram of chiral volume deviations from ideal:
255
+ 0.000 - 0.031: 40
256
+ 0.031 - 0.062: 21
257
+ 0.062 - 0.094: 13
258
+ 0.094 - 0.125: 1
259
+ 0.125 - 0.156: 1
260
+ Chirality restraints: 76
261
+ Sorted by residual:
262
+ chirality pdb=" CB ILE A1065 "
263
+ pdb=" CA ILE A1065 "
264
+ pdb=" CG1 ILE A1065 "
265
+ pdb=" CG2 ILE A1065 "
266
+ both_signs ideal model delta sigma weight residual
267
+ False 2.64 2.49 0.16 2.00e-01 2.50e+01 6.06e-01
268
+ chirality pdb=" CB ILE A1066 "
269
+ pdb=" CA ILE A1066 "
270
+ pdb=" CG1 ILE A1066 "
271
+ pdb=" CG2 ILE A1066 "
272
+ both_signs ideal model delta sigma weight residual
273
+ False 2.64 2.53 0.11 2.00e-01 2.50e+01 3.06e-01
274
+ chirality pdb=" CA TYR A1018 "
275
+ pdb=" N TYR A1018 "
276
+ pdb=" C TYR A1018 "
277
+ pdb=" CB TYR A1018 "
278
+ both_signs ideal model delta sigma weight residual
279
+ False 2.51 2.42 0.09 2.00e-01 2.50e+01 2.07e-01
280
+ ... (remaining 73 not shown)
281
+
282
+ Planarity restraints: 84
283
+ Sorted by residual:
284
+ delta sigma weight rms_deltas residual
285
+ plane pdb=" CA SER A1040 " 0.005 2.00e-02 2.50e+03 1.08e-02 1.17e+00
286
+ pdb=" C SER A1040 " -0.019 2.00e-02 2.50e+03
287
+ pdb=" O SER A1040 " 0.007 2.00e-02 2.50e+03
288
+ pdb=" N PRO A1041 " 0.006 2.00e-02 2.50e+03
289
+ delta sigma weight rms_deltas residual
290
+ plane pdb=" CD ARG A1020 " -0.010 2.00e-02 2.50e+03 9.40e-03 1.10e+00
291
+ pdb=" NE ARG A1020 " 0.016 2.00e-02 2.50e+03
292
+ pdb=" CZ ARG A1020 " -0.004 2.00e-02 2.50e+03
293
+ pdb=" NH1 ARG A1020 " 0.005 2.00e-02 2.50e+03
294
+ pdb=" NH2 ARG A1020 " -0.006 2.00e-02 2.50e+03
295
+ delta sigma weight rms_deltas residual
296
+ plane pdb=" CA GLN A1043 " 0.005 2.00e-02 2.50e+03 9.14e-03 8.35e-01
297
+ pdb=" C GLN A1043 " -0.016 2.00e-02 2.50e+03
298
+ pdb=" O GLN A1043 " 0.006 2.00e-02 2.50e+03
299
+ pdb=" N LEU A1044 " 0.005 2.00e-02 2.50e+03
300
+ ... (remaining 81 not shown)
301
+
302
+ Histogram of nonbonded interaction distances:
303
+ 2.29 - 2.81: 225
304
+ 2.81 - 3.33: 667
305
+ 3.33 - 3.86: 1265
306
+ 3.86 - 4.38: 1575
307
+ 4.38 - 4.90: 2246
308
+ Nonbonded interactions: 5978
309
+ Sorted by model distance:
310
+ nonbonded pdb=" O HOH A1131 "
311
+ pdb=" O HOH A1149 "
312
+ model vdw
313
+ 2.288 2.440
314
+ nonbonded pdb=" O HOH A1146 "
315
+ pdb=" O HOH A1151 "
316
+ model vdw
317
+ 2.297 2.440
318
+ nonbonded pdb=" O HOH A1130 "
319
+ pdb=" O HOH A1177 "
320
+ model vdw
321
+ 2.297 2.440
322
+ nonbonded pdb=" O HOH A1139 "
323
+ pdb=" O HOH A1143 "
324
+ model vdw
325
+ 2.298 2.440
326
+ nonbonded pdb=" OD2 ASP A1059 "
327
+ pdb=" O HOH A1173 "
328
+ model vdw
329
+ 2.299 2.440
330
+ ... (remaining 5973 not shown)
331
+
332
+ NOTE: a complete listing of the restraints can be obtained by requesting
333
+ output of .geo file.
334
+
335
+============================== Scattering factors =============================
336
+
337
+
338
+ ----------X-ray scattering dictionary----------
339
+
340
+Number of scattering types: 4
341
+ Type Number sf(0) Gaussians
342
+ S 3 15.96 2
343
+ O 216 7.97 2
344
+ N 85 6.97 2
345
+ C 298 5.97 2
346
+ sf(0) = scattering factor at diffraction angle 0.
347
+
348
+Number of scatterers: 602
349
+At special positions: 0
350
+Unit cell: (32.969, 38.166, 51.062, 90, 90, 90)
351
+Space group: P 21 21 21 (No. 19)
352
+
353
+ ----------F(model) initialization----------
354
+
355
+ start: r(all,work,free)=0.2720 0.2733 0.2502 n_refl.: 31449
356
+ re-set all scales: r(all,work,free)=0.2720 0.2733 0.2502 n_refl.: 31449
357
+ remove outliers: r(all,work,free)=0.2722 0.2734 0.2502 n_refl.: 31445
358
+bulk-solvent and scaling: r(all,work,free)=0.1978 0.1984 0.1864 n_refl.: 31445
359
+ remove outliers: r(all,work,free)=0.1977 0.1983 0.1864 n_refl.: 31444
360
+|-Mask optimization: start----------------------------------------------------|
361
+| Solvent (probe) radius= 1.11 Shrink truncation radius= 0.90 |
362
+| all data: 500 lowest resolution reflections: |
363
+| r_work= 0.1983 r_free= 0.1864 r_work= 0.2432 |
364
+|-----------------------------------------------------------------------------|
365
+
366
+r_solv= 0.00 r_shrink= 0.00 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
367
+r_solv= 0.10 r_shrink= 0.00 r_work=0.2008 r_free=0.1943 r_work_low=0.3020
368
+r_solv= 0.20 r_shrink= 0.00 r_work=0.2000 r_free=0.1930 r_work_low=0.2725
369
+r_solv= 0.30 r_shrink= 0.00 r_work=0.1992 r_free=0.1917 r_work_low=0.2512
370
+r_solv= 0.40 r_shrink= 0.00 r_work=0.1985 r_free=0.1902 r_work_low=0.2362
371
+r_solv= 0.50 r_shrink= 0.00 r_work=0.1982 r_free=0.1890 r_work_low=0.2416
372
+r_solv= 0.60 r_shrink= 0.00 r_work=0.1983 r_free=0.1887 r_work_low=0.2547
373
+r_solv= 0.70 r_shrink= 0.00 r_work=0.1987 r_free=0.1886 r_work_low=0.2696
374
+r_solv= 0.80 r_shrink= 0.00 r_work=0.1992 r_free=0.1890 r_work_low=0.2839
375
+r_solv= 0.90 r_shrink= 0.00 r_work=0.1998 r_free=0.1895 r_work_low=0.2974
376
+r_solv= 1.00 r_shrink= 0.00 r_work=0.2004 r_free=0.1902 r_work_low=0.3092
377
+r_solv= 1.10 r_shrink= 0.00 r_work=0.2009 r_free=0.1908 r_work_low=0.3185
378
+r_solv= 1.20 r_shrink= 0.00 r_work=0.2013 r_free=0.1915 r_work_low=0.3244
379
+r_solv= 1.30 r_shrink= 0.00 r_work=0.2017 r_free=0.1919 r_work_low=0.3282
380
+r_solv= 1.40 r_shrink= 0.00 r_work=0.2021 r_free=0.1921 r_work_low=0.3301
381
+r_solv= 0.00 r_shrink= 0.10 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
382
+r_solv= 0.10 r_shrink= 0.10 r_work=0.2008 r_free=0.1943 r_work_low=0.3020
383
+r_solv= 0.20 r_shrink= 0.10 r_work=0.2000 r_free=0.1930 r_work_low=0.2725
384
+r_solv= 0.30 r_shrink= 0.10 r_work=0.1992 r_free=0.1917 r_work_low=0.2512
385
+r_solv= 0.40 r_shrink= 0.10 r_work=0.1985 r_free=0.1902 r_work_low=0.2362
386
+r_solv= 0.50 r_shrink= 0.10 r_work=0.1982 r_free=0.1890 r_work_low=0.2416
387
+r_solv= 0.60 r_shrink= 0.10 r_work=0.1983 r_free=0.1887 r_work_low=0.2547
388
+r_solv= 0.70 r_shrink= 0.10 r_work=0.1987 r_free=0.1886 r_work_low=0.2696
389
+r_solv= 0.80 r_shrink= 0.10 r_work=0.1992 r_free=0.1890 r_work_low=0.2839
390
+r_solv= 0.90 r_shrink= 0.10 r_work=0.1998 r_free=0.1895 r_work_low=0.2974
391
+r_solv= 1.00 r_shrink= 0.10 r_work=0.2004 r_free=0.1902 r_work_low=0.3092
392
+r_solv= 1.10 r_shrink= 0.10 r_work=0.2009 r_free=0.1908 r_work_low=0.3185
393
+r_solv= 1.20 r_shrink= 0.10 r_work=0.2013 r_free=0.1915 r_work_low=0.3244
394
+r_solv= 1.30 r_shrink= 0.10 r_work=0.2017 r_free=0.1919 r_work_low=0.3282
395
+r_solv= 1.40 r_shrink= 0.10 r_work=0.2021 r_free=0.1921 r_work_low=0.3301
396
+r_solv= 0.00 r_shrink= 0.20 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
397
+r_solv= 0.10 r_shrink= 0.20 r_work=0.2008 r_free=0.1943 r_work_low=0.3020
398
+r_solv= 0.20 r_shrink= 0.20 r_work=0.2000 r_free=0.1930 r_work_low=0.2725
399
+r_solv= 0.30 r_shrink= 0.20 r_work=0.1992 r_free=0.1917 r_work_low=0.2512
400
+r_solv= 0.40 r_shrink= 0.20 r_work=0.1985 r_free=0.1902 r_work_low=0.2362
401
+r_solv= 0.50 r_shrink= 0.20 r_work=0.1982 r_free=0.1890 r_work_low=0.2416
402
+r_solv= 0.60 r_shrink= 0.20 r_work=0.1983 r_free=0.1887 r_work_low=0.2547
403
+r_solv= 0.70 r_shrink= 0.20 r_work=0.1987 r_free=0.1886 r_work_low=0.2696
404
+r_solv= 0.80 r_shrink= 0.20 r_work=0.1992 r_free=0.1890 r_work_low=0.2839
405
+r_solv= 0.90 r_shrink= 0.20 r_work=0.1998 r_free=0.1895 r_work_low=0.2974
406
+r_solv= 1.00 r_shrink= 0.20 r_work=0.2004 r_free=0.1902 r_work_low=0.3092
407
+r_solv= 1.10 r_shrink= 0.20 r_work=0.2009 r_free=0.1908 r_work_low=0.3185
408
+r_solv= 1.20 r_shrink= 0.20 r_work=0.2013 r_free=0.1915 r_work_low=0.3244
409
+r_solv= 1.30 r_shrink= 0.20 r_work=0.2017 r_free=0.1919 r_work_low=0.3282
410
+r_solv= 1.40 r_shrink= 0.20 r_work=0.2021 r_free=0.1921 r_work_low=0.3301
411
+r_solv= 0.00 r_shrink= 0.30 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
412
+r_solv= 0.10 r_shrink= 0.30 r_work=0.2016 r_free=0.1953 r_work_low=0.3304
413
+r_solv= 0.20 r_shrink= 0.30 r_work=0.2016 r_free=0.1955 r_work_low=0.3276
414
+r_solv= 0.30 r_shrink= 0.30 r_work=0.2010 r_free=0.1946 r_work_low=0.3013
415
+r_solv= 0.40 r_shrink= 0.30 r_work=0.2000 r_free=0.1932 r_work_low=0.2660
416
+r_solv= 0.50 r_shrink= 0.30 r_work=0.1990 r_free=0.1916 r_work_low=0.2412
417
+r_solv= 0.60 r_shrink= 0.30 r_work=0.1982 r_free=0.1900 r_work_low=0.2313
418
+r_solv= 0.70 r_shrink= 0.30 r_work=0.1981 r_free=0.1886 r_work_low=0.2402
419
+r_solv= 0.80 r_shrink= 0.30 r_work=0.1983 r_free=0.1881 r_work_low=0.2578
420
+r_solv= 0.90 r_shrink= 0.30 r_work=0.1988 r_free=0.1883 r_work_low=0.2731
421
+r_solv= 1.00 r_shrink= 0.30 r_work=0.1994 r_free=0.1889 r_work_low=0.2870
422
+r_solv= 1.10 r_shrink= 0.30 r_work=0.2000 r_free=0.1896 r_work_low=0.2997
423
+r_solv= 1.20 r_shrink= 0.30 r_work=0.2006 r_free=0.1904 r_work_low=0.3110
424
+r_solv= 1.30 r_shrink= 0.30 r_work=0.2010 r_free=0.1910 r_work_low=0.3207
425
+r_solv= 1.40 r_shrink= 0.30 r_work=0.2014 r_free=0.1916 r_work_low=0.3262
426
+r_solv= 0.00 r_shrink= 0.40 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
427
+r_solv= 0.10 r_shrink= 0.40 r_work=0.2016 r_free=0.1952 r_work_low=0.3305
428
+r_solv= 0.20 r_shrink= 0.40 r_work=0.2016 r_free=0.1953 r_work_low=0.3299
429
+r_solv= 0.30 r_shrink= 0.40 r_work=0.2017 r_free=0.1956 r_work_low=0.3277
430
+r_solv= 0.40 r_shrink= 0.40 r_work=0.2010 r_free=0.1948 r_work_low=0.2980
431
+r_solv= 0.50 r_shrink= 0.40 r_work=0.1999 r_free=0.1930 r_work_low=0.2610
432
+r_solv= 0.60 r_shrink= 0.40 r_work=0.1988 r_free=0.1914 r_work_low=0.2377
433
+r_solv= 0.70 r_shrink= 0.40 r_work=0.1981 r_free=0.1896 r_work_low=0.2319
434
+r_solv= 0.80 r_shrink= 0.40 r_work=0.1981 r_free=0.1880 r_work_low=0.2434
435
+r_solv= 0.90 r_shrink= 0.40 r_work=0.1984 r_free=0.1879 r_work_low=0.2597
436
+r_solv= 1.00 r_shrink= 0.40 r_work=0.1990 r_free=0.1882 r_work_low=0.2751
437
+r_solv= 1.10 r_shrink= 0.40 r_work=0.1995 r_free=0.1889 r_work_low=0.2880
438
+r_solv= 1.20 r_shrink= 0.40 r_work=0.2001 r_free=0.1897 r_work_low=0.3000
439
+r_solv= 1.30 r_shrink= 0.40 r_work=0.2006 r_free=0.1904 r_work_low=0.3123
440
+r_solv= 1.40 r_shrink= 0.40 r_work=0.2011 r_free=0.1911 r_work_low=0.3218
441
+r_solv= 0.00 r_shrink= 0.50 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
442
+r_solv= 0.10 r_shrink= 0.50 r_work=0.2016 r_free=0.1952 r_work_low=0.3305
443
+r_solv= 0.20 r_shrink= 0.50 r_work=0.2016 r_free=0.1953 r_work_low=0.3301
444
+r_solv= 0.30 r_shrink= 0.50 r_work=0.2017 r_free=0.1956 r_work_low=0.3301
445
+r_solv= 0.40 r_shrink= 0.50 r_work=0.2014 r_free=0.1957 r_work_low=0.3131
446
+r_solv= 0.50 r_shrink= 0.50 r_work=0.2004 r_free=0.1938 r_work_low=0.2737
447
+r_solv= 0.60 r_shrink= 0.50 r_work=0.1992 r_free=0.1921 r_work_low=0.2436
448
+r_solv= 0.70 r_shrink= 0.50 r_work=0.1983 r_free=0.1900 r_work_low=0.2321
449
+r_solv= 0.80 r_shrink= 0.50 r_work=0.1981 r_free=0.1883 r_work_low=0.2383
450
+r_solv= 0.90 r_shrink= 0.50 r_work=0.1983 r_free=0.1877 r_work_low=0.2530
451
+r_solv= 1.00 r_shrink= 0.50 r_work=0.1988 r_free=0.1878 r_work_low=0.2690
452
+r_solv= 1.10 r_shrink= 0.50 r_work=0.1993 r_free=0.1885 r_work_low=0.2827
453
+r_solv= 1.20 r_shrink= 0.50 r_work=0.1999 r_free=0.1894 r_work_low=0.2945
454
+r_solv= 1.30 r_shrink= 0.50 r_work=0.2004 r_free=0.1901 r_work_low=0.3078
455
+r_solv= 1.40 r_shrink= 0.50 r_work=0.2009 r_free=0.1909 r_work_low=0.3188
456
+r_solv= 0.00 r_shrink= 0.60 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
457
+r_solv= 0.10 r_shrink= 0.60 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
458
+r_solv= 0.20 r_shrink= 0.60 r_work=0.2016 r_free=0.1952 r_work_low=0.3304
459
+r_solv= 0.30 r_shrink= 0.60 r_work=0.2017 r_free=0.1955 r_work_low=0.3325
460
+r_solv= 0.40 r_shrink= 0.60 r_work=0.2018 r_free=0.1962 r_work_low=0.3309
461
+r_solv= 0.50 r_shrink= 0.60 r_work=0.2014 r_free=0.1959 r_work_low=0.3076
462
+r_solv= 0.60 r_shrink= 0.60 r_work=0.2005 r_free=0.1946 r_work_low=0.2727
463
+r_solv= 0.70 r_shrink= 0.60 r_work=0.1993 r_free=0.1918 r_work_low=0.2444
464
+r_solv= 0.80 r_shrink= 0.60 r_work=0.1984 r_free=0.1898 r_work_low=0.2395
465
+r_solv= 0.90 r_shrink= 0.60 r_work=0.1981 r_free=0.1881 r_work_low=0.2414
466
+r_solv= 1.00 r_shrink= 0.60 r_work=0.1984 r_free=0.1870 r_work_low=0.2535
467
+r_solv= 1.10 r_shrink= 0.60 r_work=0.1988 r_free=0.1876 r_work_low=0.2667
468
+r_solv= 1.20 r_shrink= 0.60 r_work=0.1994 r_free=0.1885 r_work_low=0.2799
469
+r_solv= 1.30 r_shrink= 0.60 r_work=0.1999 r_free=0.1892 r_work_low=0.2932
470
+r_solv= 1.40 r_shrink= 0.60 r_work=0.2004 r_free=0.1902 r_work_low=0.3069
471
+r_solv= 0.00 r_shrink= 0.70 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
472
+r_solv= 0.10 r_shrink= 0.70 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
473
+r_solv= 0.20 r_shrink= 0.70 r_work=0.2016 r_free=0.1952 r_work_low=0.3305
474
+r_solv= 0.30 r_shrink= 0.70 r_work=0.2017 r_free=0.1954 r_work_low=0.3325
475
+r_solv= 0.40 r_shrink= 0.70 r_work=0.2018 r_free=0.1962 r_work_low=0.3342
476
+r_solv= 0.50 r_shrink= 0.70 r_work=0.2016 r_free=0.1961 r_work_low=0.3168
477
+r_solv= 0.60 r_shrink= 0.70 r_work=0.2009 r_free=0.1956 r_work_low=0.2864
478
+r_solv= 0.70 r_shrink= 0.70 r_work=0.1997 r_free=0.1925 r_work_low=0.2547
479
+r_solv= 0.80 r_shrink= 0.70 r_work=0.1987 r_free=0.1904 r_work_low=0.2429
480
+r_solv= 0.90 r_shrink= 0.70 r_work=0.1982 r_free=0.1885 r_work_low=0.2420
481
+r_solv= 1.00 r_shrink= 0.70 r_work=0.1983 r_free=0.1868 r_work_low=0.2488
482
+r_solv= 1.10 r_shrink= 0.70 r_work=0.1987 r_free=0.1873 r_work_low=0.2599
483
+r_solv= 1.20 r_shrink= 0.70 r_work=0.1992 r_free=0.1882 r_work_low=0.2745
484
+r_solv= 1.30 r_shrink= 0.70 r_work=0.1997 r_free=0.1889 r_work_low=0.2882
485
+r_solv= 1.40 r_shrink= 0.70 r_work=0.2002 r_free=0.1898 r_work_low=0.3019
486
+r_solv= 0.00 r_shrink= 0.80 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
487
+r_solv= 0.10 r_shrink= 0.80 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
488
+r_solv= 0.20 r_shrink= 0.80 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
489
+r_solv= 0.30 r_shrink= 0.80 r_work=0.2017 r_free=0.1953 r_work_low=0.3325
490
+r_solv= 0.40 r_shrink= 0.80 r_work=0.2019 r_free=0.1961 r_work_low=0.3376
491
+r_solv= 0.50 r_shrink= 0.80 r_work=0.2018 r_free=0.1962 r_work_low=0.3280
492
+r_solv= 0.60 r_shrink= 0.80 r_work=0.2013 r_free=0.1965 r_work_low=0.3023
493
+r_solv= 0.70 r_shrink= 0.80 r_work=0.2006 r_free=0.1946 r_work_low=0.2769
494
+r_solv= 0.80 r_shrink= 0.80 r_work=0.1996 r_free=0.1917 r_work_low=0.2647
495
+r_solv= 0.90 r_shrink= 0.80 r_work=0.1986 r_free=0.1894 r_work_low=0.2530
496
+r_solv= 1.00 r_shrink= 0.80 r_work=0.1983 r_free=0.1870 r_work_low=0.2479
497
+r_solv= 1.10 r_shrink= 0.80 r_work=0.1984 r_free=0.1866 r_work_low=0.2483
498
+r_solv= 1.20 r_shrink= 0.80 r_work=0.1988 r_free=0.1873 r_work_low=0.2619
499
+r_solv= 1.30 r_shrink= 0.80 r_work=0.1994 r_free=0.1881 r_work_low=0.2782
500
+r_solv= 1.40 r_shrink= 0.80 r_work=0.1999 r_free=0.1891 r_work_low=0.2922
501
+r_solv= 0.00 r_shrink= 0.90 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
502
+r_solv= 0.10 r_shrink= 0.90 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
503
+r_solv= 0.20 r_shrink= 0.90 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
504
+r_solv= 0.30 r_shrink= 0.90 r_work=0.2016 r_free=0.1953 r_work_low=0.3318
505
+r_solv= 0.40 r_shrink= 0.90 r_work=0.2019 r_free=0.1960 r_work_low=0.3386
506
+r_solv= 0.50 r_shrink= 0.90 r_work=0.2019 r_free=0.1963 r_work_low=0.3345
507
+r_solv= 0.60 r_shrink= 0.90 r_work=0.2016 r_free=0.1968 r_work_low=0.3126
508
+r_solv= 0.70 r_shrink= 0.90 r_work=0.2011 r_free=0.1955 r_work_low=0.2890
509
+r_solv= 0.80 r_shrink= 0.90 r_work=0.2002 r_free=0.1933 r_work_low=0.2820
510
+r_solv= 0.90 r_shrink= 0.90 r_work=0.1991 r_free=0.1904 r_work_low=0.2658
511
+r_solv= 1.00 r_shrink= 0.90 r_work=0.1984 r_free=0.1873 r_work_low=0.2538
512
+r_solv= 1.10 r_shrink= 0.90 r_work=0.1983 r_free=0.1866 r_work_low=0.2429
513
+r_solv= 1.20 r_shrink= 0.90 r_work=0.1986 r_free=0.1869 r_work_low=0.2538
514
+r_solv= 1.30 r_shrink= 0.90 r_work=0.1991 r_free=0.1875 r_work_low=0.2702
515
+r_solv= 1.40 r_shrink= 0.90 r_work=0.1996 r_free=0.1886 r_work_low=0.2851
516
+r_solv= 0.00 r_shrink= 1.00 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
517
+r_solv= 0.10 r_shrink= 1.00 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
518
+r_solv= 0.20 r_shrink= 1.00 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
519
+r_solv= 0.30 r_shrink= 1.00 r_work=0.2016 r_free=0.1953 r_work_low=0.3312
520
+r_solv= 0.40 r_shrink= 1.00 r_work=0.2019 r_free=0.1960 r_work_low=0.3388
521
+r_solv= 0.50 r_shrink= 1.00 r_work=0.2019 r_free=0.1962 r_work_low=0.3390
522
+r_solv= 0.60 r_shrink= 1.00 r_work=0.2017 r_free=0.1970 r_work_low=0.3216
523
+r_solv= 0.70 r_shrink= 1.00 r_work=0.2014 r_free=0.1961 r_work_low=0.3012
524
+r_solv= 0.80 r_shrink= 1.00 r_work=0.2007 r_free=0.1945 r_work_low=0.2936
525
+r_solv= 0.90 r_shrink= 1.00 r_work=0.1997 r_free=0.1917 r_work_low=0.2852
526
+r_solv= 1.00 r_shrink= 1.00 r_work=0.1988 r_free=0.1878 r_work_low=0.2655
527
+r_solv= 1.10 r_shrink= 1.00 r_work=0.1984 r_free=0.1868 r_work_low=0.2433
528
+r_solv= 1.20 r_shrink= 1.00 r_work=0.1985 r_free=0.1865 r_work_low=0.2470
529
+r_solv= 1.30 r_shrink= 1.00 r_work=0.1989 r_free=0.1869 r_work_low=0.2628
530
+r_solv= 1.40 r_shrink= 1.00 r_work=0.1994 r_free=0.1881 r_work_low=0.2771
531
+r_solv= 0.00 r_shrink= 1.10 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
532
+r_solv= 0.10 r_shrink= 1.10 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
533
+r_solv= 0.20 r_shrink= 1.10 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
534
+r_solv= 0.30 r_shrink= 1.10 r_work=0.2016 r_free=0.1952 r_work_low=0.3308
535
+r_solv= 0.40 r_shrink= 1.10 r_work=0.2018 r_free=0.1959 r_work_low=0.3383
536
+r_solv= 0.50 r_shrink= 1.10 r_work=0.2020 r_free=0.1962 r_work_low=0.3411
537
+r_solv= 0.60 r_shrink= 1.10 r_work=0.2018 r_free=0.1971 r_work_low=0.3285
538
+r_solv= 0.70 r_shrink= 1.10 r_work=0.2017 r_free=0.1966 r_work_low=0.3122
539
+r_solv= 0.80 r_shrink= 1.10 r_work=0.2011 r_free=0.1954 r_work_low=0.3052
540
+r_solv= 0.90 r_shrink= 1.10 r_work=0.2002 r_free=0.1932 r_work_low=0.3026
541
+r_solv= 1.00 r_shrink= 1.10 r_work=0.1994 r_free=0.1883 r_work_low=0.2830
542
+r_solv= 1.10 r_shrink= 1.10 r_work=0.1986 r_free=0.1868 r_work_low=0.2513
543
+r_solv= 1.20 r_shrink= 1.10 r_work=0.1984 r_free=0.1868 r_work_low=0.2434
544
+r_solv= 1.30 r_shrink= 1.10 r_work=0.1987 r_free=0.1866 r_work_low=0.2542
545
+r_solv= 1.40 r_shrink= 1.10 r_work=0.1992 r_free=0.1873 r_work_low=0.2684
546
+r_solv= 0.00 r_shrink= 1.20 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
547
+r_solv= 0.10 r_shrink= 1.20 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
548
+r_solv= 0.20 r_shrink= 1.20 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
549
+r_solv= 0.30 r_shrink= 1.20 r_work=0.2016 r_free=0.1952 r_work_low=0.3307
550
+r_solv= 0.40 r_shrink= 1.20 r_work=0.2018 r_free=0.1957 r_work_low=0.3374
551
+r_solv= 0.50 r_shrink= 1.20 r_work=0.2020 r_free=0.1961 r_work_low=0.3417
552
+r_solv= 0.60 r_shrink= 1.20 r_work=0.2019 r_free=0.1970 r_work_low=0.3333
553
+r_solv= 0.70 r_shrink= 1.20 r_work=0.2019 r_free=0.1968 r_work_low=0.3196
554
+r_solv= 0.80 r_shrink= 1.20 r_work=0.2013 r_free=0.1960 r_work_low=0.3114
555
+r_solv= 0.90 r_shrink= 1.20 r_work=0.2005 r_free=0.1942 r_work_low=0.3138
556
+r_solv= 1.00 r_shrink= 1.20 r_work=0.1997 r_free=0.1889 r_work_low=0.2941
557
+r_solv= 1.10 r_shrink= 1.20 r_work=0.1989 r_free=0.1870 r_work_low=0.2617
558
+r_solv= 1.20 r_shrink= 1.20 r_work=0.1985 r_free=0.1871 r_work_low=0.2457
559
+r_solv= 1.30 r_shrink= 1.20 r_work=0.1985 r_free=0.1864 r_work_low=0.2471
560
+r_solv= 1.40 r_shrink= 1.20 r_work=0.1991 r_free=0.1870 r_work_low=0.2634
561
+r_solv= 0.00 r_shrink= 1.30 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
562
+r_solv= 0.10 r_shrink= 1.30 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
563
+r_solv= 0.20 r_shrink= 1.30 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
564
+r_solv= 0.30 r_shrink= 1.30 r_work=0.2016 r_free=0.1952 r_work_low=0.3307
565
+r_solv= 0.40 r_shrink= 1.30 r_work=0.2018 r_free=0.1957 r_work_low=0.3370
566
+r_solv= 0.50 r_shrink= 1.30 r_work=0.2020 r_free=0.1960 r_work_low=0.3418
567
+r_solv= 0.60 r_shrink= 1.30 r_work=0.2019 r_free=0.1970 r_work_low=0.3358
568
+r_solv= 0.70 r_shrink= 1.30 r_work=0.2019 r_free=0.1970 r_work_low=0.3237
569
+r_solv= 0.80 r_shrink= 1.30 r_work=0.2015 r_free=0.1965 r_work_low=0.3155
570
+r_solv= 0.90 r_shrink= 1.30 r_work=0.2007 r_free=0.1950 r_work_low=0.3221
571
+r_solv= 1.00 r_shrink= 1.30 r_work=0.1999 r_free=0.1895 r_work_low=0.3035
572
+r_solv= 1.10 r_shrink= 1.30 r_work=0.1991 r_free=0.1872 r_work_low=0.2676
573
+r_solv= 1.20 r_shrink= 1.30 r_work=0.1986 r_free=0.1874 r_work_low=0.2504
574
+r_solv= 1.30 r_shrink= 1.30 r_work=0.1984 r_free=0.1864 r_work_low=0.2449
575
+r_solv= 1.40 r_shrink= 1.30 r_work=0.1990 r_free=0.1868 r_work_low=0.2594
576
+r_solv= 0.00 r_shrink= 1.40 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
577
+r_solv= 0.10 r_shrink= 1.40 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
578
+r_solv= 0.20 r_shrink= 1.40 r_work=0.2015 r_free=0.1952 r_work_low=0.3306
579
+r_solv= 0.30 r_shrink= 1.40 r_work=0.2016 r_free=0.1952 r_work_low=0.3306
580
+r_solv= 0.40 r_shrink= 1.40 r_work=0.2017 r_free=0.1955 r_work_low=0.3357
581
+r_solv= 0.50 r_shrink= 1.40 r_work=0.2019 r_free=0.1959 r_work_low=0.3411
582
+r_solv= 0.60 r_shrink= 1.40 r_work=0.2019 r_free=0.1968 r_work_low=0.3389
583
+r_solv= 0.70 r_shrink= 1.40 r_work=0.2020 r_free=0.1972 r_work_low=0.3300
584
+r_solv= 0.80 r_shrink= 1.40 r_work=0.2017 r_free=0.1971 r_work_low=0.3218
585
+r_solv= 0.90 r_shrink= 1.40 r_work=0.2011 r_free=0.1960 r_work_low=0.3323
586
+r_solv= 1.00 r_shrink= 1.40 r_work=0.2003 r_free=0.1905 r_work_low=0.3169
587
+r_solv= 1.10 r_shrink= 1.40 r_work=0.1995 r_free=0.1881 r_work_low=0.2785
588
+r_solv= 1.20 r_shrink= 1.40 r_work=0.1989 r_free=0.1874 r_work_low=0.2593
589
+r_solv= 1.30 r_shrink= 1.40 r_work=0.1984 r_free=0.1866 r_work_low=0.2447
590
+r_solv= 1.40 r_shrink= 1.40 r_work=0.1989 r_free=0.1866 r_work_low=0.2549
591
+
592
+|-Mask optimization: final----------------------------------------------------|
593
+| Solvent (probe) radius= 0.70 Shrink truncation radius= 0.30 |
594
+| all data: 500 lowest resolution reflections: |
595
+| r_work= 0.1981 r_free= 0.1886 r_work= 0.2402 |
596
+|-----------------------------------------------------------------------------|
597
+
598
+|--(resolution: 1.04 - 19.08 A, n_refl.=31444 (all), 4.96 % free)------------|
599
+| |
600
+| r_work= 0.1981 r_free= 0.1886 coordinate error (max.-lik. estimate): 0.09 A |
601
+| |
602
+| normalized target function (ml) (work): 4.640880 |
603
+| target function (ml) not normalized (work): 138683.431375 |
604
+| target function (ml) not normalized (free): 7189.821067 |
605
+|-----------------------------------------------------------------------------|
606
+
607
+End of input processing
608
+
609
+======================= ROSETTA/PHENIX X-ray refinement =======================
610
+
611
+Output directory:
612
+ /nfs/staff/key/software_tests/PHENIX.ROSETTA.REFINE_linux/rosetta_refine_4
613
+
614
+ ----------Setting up input files for Rosetta----------
615
+
616
+|-starting model--------------------------------------------------------------|
617
+| target_work(ml) = 4.64088 r_work = 0.1981 r_free = 0.1886 |
618
+|-----------------------------------------------------------------------------|
619
+
620
+ Validation statistics (starting model):
621
+ Ramachandran outliers = 0.00 %
622
+ favored = 100.00 %
623
+ Rotamer outliers = 2.04 %
624
+ C-beta deviations = 0
625
+ Clashscore = 4.15
626
+ RMS(bonds) = 0.0000
627
+ RMS(angles) = 0.00
628
+ MolProbity score = 1.43
629
+
630
+
631
+Rosetta command-line arguments:
632
+ -parser:protocol /programs/x86_64-linux/rosetta/3.8/main/source/src/apps/public/crystal_refinement/low_resolution_refine.xml
633
+ -s 1I2T_modified_rosetta_in.pdb
634
+ -mtzfile 1I2T_modified_rosetta_data.mtz
635
+ -run:preserve_header
636
+ -crystal_refine
637
+ -parser:script_vars symmdef=1I2T_modified_rosetta.symm
638
+ -parser:script_vars bfactstrat=individual
639
+ -parser:script_vars map_type=Auto
640
+ -score:weights talaris2013_cart
641
+ -nstruct 1
642
+ -database /programs/x86_64-linux/rosetta/3.8/main/database
643
+
644
+Generating 5 models on 1 processors...
645
+
646
+ 1: r_work = 0.2200 r_free = 0.2181 energy = -694.96 rmsd = 0.946 ***
647
+ 2: r_work = 0.2207 r_free = 0.2171 energy = -698.52 rmsd = 1.065 ***
648
+ 3: r_work = 0.2206 r_free = 0.2139 energy = -704.21 rmsd = 0.970 ***
649
+ 4: r_work = 0.2199 r_free = 0.2152 energy = -711.36 rmsd = 1.001
650
+ 5: r_work = 0.2231 r_free = 0.2205 energy = -703.18 rmsd = 1.156
651
+
652
+|-after ROSETTA---------------------------------------------------------------|
653
+| target_work(ml) = 4.64366 r_work = 0.2206 r_free = 0.2139 |
654
+|-----------------------------------------------------------------------------|
655
+
656
+ Validation statistics after ROSETTA:
657
+ Ramachandran outliers = 0.00 %
658
+ favored = 100.00 %
659
+ Rotamer outliers = 0.00 %
660
+ C-beta deviations = 0
661
+ Clashscore = 0.00
662
+ RMS(bonds) = 0.0000
663
+ RMS(angles) = 0.00
664
+ MolProbity score = 0.50
665
+
666
+
667
+ ----------Running phenix.refine (with null strategy)----------
668
+
669
+start r_work=0.2898 r_free=0.2737
670
+1_bss r_work=0.2120 r_free=0.2065
671
+end r_work=0.2120 r_free=0.2065
672
+ Ramachandran outliers = 0.00 %
673
+ favored = 100.00 %
674
+ Rotamer outliers = 0.00 %
675
+ C-beta deviations = 0
676
+ Clashscore = 9.34
677
+ RMS(bonds) = 0.1003
678
+ RMS(angles) = 1.77
679
+ MolProbity score = 1.49
680
+ Resolution = 1.04
681
+ R-work = 0.2120
682
+ R-free = 0.2065
683
+
684
+ ----------Final results----------
685
+
686
+
687
+Refined model: 1I2T_modified_rosetta_phenix_001.pdb
688
+Final maps: 1I2T_modified_rosetta_phenix_001.mtz
689
+
690
+Elapsed time: 9291.2s
691
+
692
+Citation:
693
+
694
+DiMaio F., Echols N., Headd J.J., Terwilliger T.C., Adams P.D., and Baker D.
695
+(2013). Improved low-resolution crystallographic refinement with Phenix and
696
+Rosetta. Nat Methods 10, 1102-4.
697
+
examples/phenix.rosetta_refine.md
... ...
@@ -1 +1,31 @@
1
-##coming soon
1
+## Running PHENIX with Rosetta
2
+
3
+Running PHENIX with Rosetta requires compatible versions of PHENIX and Rosetta to be installed and enabled in the shell environment. In the SBGrid environment, the default versions of Rosetta and PHENIX are compatible and tested. Other versions may also work together (nightly builds), but we don't typically test all possible combinations.
4
+
5
+### PHENIX regression test
6
+
7
+A quick check of PHENIX Rosetta integration can be made with the phenix_regression.test_rosetta_refine command.
8
+
9
+ phenix_regression.test_rosetta_refine
10
+
11
+A successful test will output this :
12
+
13
+```
14
+$ phenix_regression.test_rosetta_refine
15
+/programs/x86_64-linux/rosetta/3.8/main/source
16
+OK
17
+```
18
+
19
+### phenix.rosetta_refine
20
+
21
+phenix.rosetta_refine can be run from the GUI or from the command line.
22
+
23
+We test rosetta with a small 61 aminoacid protein (1I2T, Poly-A binding protein, PABP).
24
+Our test dataset is available here : [1I2T.tar.bz2](1I2T.tar.bz2)
25
+
26
+This command should run to completion :
27
+
28
+ phenix.rosetta_refine 1I2T.pdb 1I2T_F.mtz protocol=hires nproc=8
29
+
30
+Here is the expected log output.
31
+[phenix.rosetta_refine.log](phenix.rosetta_refine.log)