从日志文件中提取特定的数据行
[英]Extracting specific lines of data from a log file
问题描述
I'm looking to extract and print a specific line from a table I have in a long log file. 
我想从一个长日志文件中的表中提取并打印一个特定的行。 It looks something like this: 它看起来像这样：
******************************************************************************
XSCALE (VERSION July 4, 2012) 4-Jun-2013
******************************************************************************
Author: Wolfgang Kabsch
Copy licensed until 30-Jun-2013 to
academic users for non-commercial applications
No redistribution.
******************************************************************************
CONTROL CARDS
******************************************************************************
MAXIMUM_NUMBER_OF_PROCESSORS=16
RESOLUTION_SHELLS= 20 10 6 4 3 2.5 2.0 1.9 1.8 1.7 1.6 1.5 1.4 1.3 1.2 1.1 1.0 0.9 0.8
MINIMUM_I/SIGMA=4.0
OUTPUT_FILE=fae-ip.ahkl
INPUT_FILE= /dls/sci-scratch/Sam/FC59251/fr6_1/XDS_ASCII.HKL
THE DATA COLLECTION STATISTICS REPORTED BELOW ASSUMES:
SPACE_GROUP_NUMBER= 97
UNIT_CELL_CONSTANTS= 128.28 128.28 181.47 90.000 90.000 90.000
***** 16 EQUIVALENT POSITIONS IN SPACE GROUP # 97 *****
If x',y',z' is an equivalent position to x,y,z, then
x'=x*ML(1)+y*ML( 2)+z*ML( 3)+ML( 4)/12.0
y'=x*ML(5)+y*ML( 6)+z*ML( 7)+ML( 8)/12.0
z'=x*ML(9)+y*ML(10)+z*ML(11)+ML(12)/12.0
# 1 2 3 4 5 6 7 8 9 10 11 12
1 1 0 0 0 0 1 0 0 0 0 1 0
2 -1 0 0 0 0 -1 0 0 0 0 1 0
3 -1 0 0 0 0 1 0 0 0 0 -1 0
4 1 0 0 0 0 -1 0 0 0 0 -1 0
5 0 1 0 0 1 0 0 0 0 0 -1 0
6 0 -1 0 0 -1 0 0 0 0 0 -1 0
7 0 -1 0 0 1 0 0 0 0 0 1 0
8 0 1 0 0 -1 0 0 0 0 0 1 0
9 1 0 0 6 0 1 0 6 0 0 1 6
10 -1 0 0 6 0 -1 0 6 0 0 1 6
11 -1 0 0 6 0 1 0 6 0 0 -1 6
12 1 0 0 6 0 -1 0 6 0 0 -1 6
13 0 1 0 6 1 0 0 6 0 0 -1 6
14 0 -1 0 6 -1 0 0 6 0 0 -1 6
15 0 -1 0 6 1 0 0 6 0 0 1 6
16 0 1 0 6 -1 0 0 6 0 0 1 6
ALL DATA SETS WILL BE SCALED TO /dls/sci-scratch/Sam/FC59251/fr6_1/XDS_ASCII.HKL
******************************************************************************
READING INPUT REFLECTION DATA FILES
******************************************************************************
DATA MEAN REFLECTIONS INPUT FILE NAME
SET# INTENSITY ACCEPTED REJECTED
1 0.1358E+03 1579957 0 /dls/sci-scratch/Sam/FC59251/fr6_1/XDS_ASCII.HKL
******************************************************************************
CORRECTION FACTORS AS FUNCTION OF IMAGE NUMBER & RESOLUTION
******************************************************************************
RECIPROCAL CORRECTION FACTORS FOR INPUT DATA SETS MERGED TO
OUTPUT FILE: fae-ip.ahkl
THE CALCULATIONS ASSUME FRIEDEL'S_LAW= TRUE
TOTAL NUMBER OF CORRECTION FACTORS DEFINED 720
DEGREES OF FREEDOM OF CHI^2 FIT 357222.9
CHI^2-VALUE OF FIT OF CORRECTION FACTORS 1.024
NUMBER OF CYCLES CARRIED OUT 4
CORRECTION FACTORS for visual inspection by XDS-Viewer DECAY_001.cbf
XMIN= 0.6 XMAX= 1799.3 NXBIN= 36
YMIN= 0.00049 YMAX= 0.44483 NYBIN= 20
NUMBER OF REFLECTIONS USED FOR DETERMINING CORRECTION FACTORS 396046
******************************************************************************
CORRECTION FACTORS AS FUNCTION OF X (fast) & Y(slow) IN THE DETECTOR PLANE
******************************************************************************
RECIPROCAL CORRECTION FACTORS FOR INPUT DATA SETS MERGED TO
OUTPUT FILE: fae-ip.ahkl
THE CALCULATIONS ASSUME FRIEDEL'S_LAW= TRUE
TOTAL NUMBER OF CORRECTION FACTORS DEFINED 7921
DEGREES OF FREEDOM OF CHI^2 FIT 356720.6
CHI^2-VALUE OF FIT OF CORRECTION FACTORS 1.023
NUMBER OF CYCLES CARRIED OUT 3
CORRECTION FACTORS for visual inspection by XDS-Viewer MODPIX_001.cbf
XMIN= 5.4 XMAX= 2457.6 NXBIN= 89
YMIN= 40.0 YMAX= 2516.7 NYBIN= 89
NUMBER OF REFLECTIONS USED FOR DETERMINING CORRECTION FACTORS 396046
******************************************************************************
CORRECTION FACTORS AS FUNCTION OF IMAGE NUMBER & DETECTOR SURFACE POSITION
******************************************************************************
RECIPROCAL CORRECTION FACTORS FOR INPUT DATA SETS MERGED TO
OUTPUT FILE: fae-ip.ahkl
THE CALCULATIONS ASSUME FRIEDEL'S_LAW= TRUE
TOTAL NUMBER OF CORRECTION FACTORS DEFINED 468
DEGREES OF FREEDOM OF CHI^2 FIT 357286.9
CHI^2-VALUE OF FIT OF CORRECTION FACTORS 1.022
NUMBER OF CYCLES CARRIED OUT 3
CORRECTION FACTORS for visual inspection by XDS-Viewer ABSORP_001.cbf
XMIN= 0.6 XMAX= 1799.3 NXBIN= 36
DETECTOR_SURFACE_POSITION= 1232 1278
DETECTOR_SURFACE_POSITION= 1648 1699
DETECTOR_SURFACE_POSITION= 815 1699
DETECTOR_SURFACE_POSITION= 815 858
DETECTOR_SURFACE_POSITION= 1648 858
DETECTOR_SURFACE_POSITION= 2174 1673
DETECTOR_SURFACE_POSITION= 1622 2230
DETECTOR_SURFACE_POSITION= 841 2230
DETECTOR_SURFACE_POSITION= 289 1673
DETECTOR_SURFACE_POSITION= 289 884
DETECTOR_SURFACE_POSITION= 841 326
DETECTOR_SURFACE_POSITION= 1622 326
DETECTOR_SURFACE_POSITION= 2174 884
NUMBER OF REFLECTIONS USED FOR DETERMINING CORRECTION FACTORS 396046
******************************************************************************
CORRECTION PARAMETERS FOR THE STANDARD ERROR OF REFLECTION INTENSITIES
******************************************************************************
The variance v0(I) of the intensity I obtained from counting statistics is
replaced by v(I)=a*(v0(I)+b*I^2). The model parameters a, b are chosen to
minimize the discrepancies between v(I) and the variance estimated from
sample statistics of symmetry related reflections. This model implicates
an asymptotic limit ISa=1/SQRT(a*b) for the highest I/Sigma(I) that the
experimental setup can produce (Diederichs (2010) Acta Cryst D66, 733-740).
Often the value of ISa is reduced from the initial value ISa0 due to systematic
errors showing up by comparison with other data sets in the scaling procedure.
(ISa=ISa0=-1 if v0 is unknown for a data set.)
a b ISa ISa0 INPUT DATA SET
1.086E+00 1.420E-03 25.46 29.00 /dls/sci-scratch/Sam/FC59251/fr6_1/XDS_ASCII.HKL
FACTOR TO PLACE ALL DATA SETS TO AN APPROXIMATE ABSOLUTE SCALE 0.4178E+04
(ASSUMING A PROTEIN WITH 50% SOLVENT)
******************************************************************************
STATISTICS OF SCALED OUTPUT DATA SET : fae-ip.ahkl
FILE TYPE: XDS_ASCII MERGE=FALSE FRIEDEL'S_LAW=TRUE
186 OUT OF 1579957 REFLECTIONS REJECTED
1579771 REFLECTIONS ON OUTPUT FILE
******************************************************************************
DEFINITIONS:
R-FACTOR
observed = (SUM(ABS(I(h,i)-I(h))))/(SUM(I(h,i)))
expected = expected R-FACTOR derived from Sigma(I)
COMPARED = number of reflections used for calculating R-FACTOR
I/SIGMA = mean of intensity/Sigma(I) of unique reflections
(after merging symmetry-related observations)
Sigma(I) = standard deviation of reflection intensity I
estimated from sample statistics
R-meas = redundancy independent R-factor (intensities)
Diederichs & Karplus (1997), Nature Struct. Biol. 4, 269-275.
CC(1/2) = percentage of correlation between intensities from
random half-datasets. Correlation significant at
the 0.1% level is marked by an asterisk.
Karplus & Diederichs (2012), Science 336, 1030-33
Anomal = percentage of correlation between random half-sets
Corr of anomalous intensity differences. Correlation
significant at the 0.1% level is marked.
SigAno = mean anomalous difference in units of its estimated
standard deviation (|F(+)-F(-)|/Sigma). F(+), F(-)
are structure factor estimates obtained from the
merged intensity observations in each parity class.
Nano = Number of unique reflections used to calculate
Anomal_Corr & SigAno. At least two observations
for each (+ and -) parity are required.
SUBSET OF INTENSITY DATA WITH SIGNAL/NOISE >= -3.0 AS FUNCTION OF RESOLUTION
RESOLUTION NUMBER OF REFLECTIONS COMPLETENESS R-FACTOR R-FACTOR COMPARED I/SIGMA R-meas CC(1/2) Anomal SigAno Nano
LIMIT OBSERVED UNIQUE POSSIBLE OF DATA observed expected Corr
20.00 557 66 74 89.2% 2.7% 3.0% 557 58.75 2.9% 100.0* 45 1.674 25
10.00 5018 417 417 100.0% 2.4% 3.1% 5018 75.34 2.6% 100.0* 2 0.812 276
6.00 18352 1583 1584 99.9% 2.8% 3.3% 18351 65.55 2.9% 100.0* 11* 0.914 1248
4.00 59691 4640 4640 100.0% 3.2% 3.5% 59690 64.96 3.4% 100.0* 4 0.857 3987
3.00 112106 8821 8822 100.0% 4.4% 4.4% 112102 50.31 4.6% 99.9* -3 0.844 7906
2.50 147954 11023 11023 100.0% 8.7% 8.6% 147954 29.91 9.1% 99.8* 0 0.829 10096
2.00 332952 24698 24698 100.0% 21.4% 21.6% 332949 14.32 22.3% 99.2* 1 0.804 22992
1.90 106645 8382 8384 100.0% 56.5% 57.1% 106645 5.63 58.8% 94.7* -2 0.767 7886
1.80 138516 10342 10343 100.0% 86.8% 87.0% 138516 3.64 90.2% 87.9* -2 0.762 9741
1.70 175117 12897 12899 100.0% 140.0% 140.1% 175116 2.15 145.4% 69.6* -2 0.732 12188
1.60 209398 16298 16304 100.0% 206.1% 208.5% 209397 1.35 214.6% 48.9* -2 0.693 15466
1.50 273432 20770 20893 99.4% 333.4% 342.1% 273340 0.80 346.9% 23.2* -1 0.644 19495
1.40 33 27 27248 0.1% 42.6% 112.7% 12 0.40 60.3% 88.2 0 0.000 0
1.30 0 0 36205 0.0% -99.9% -99.9% 0 -99.00 -99.9% 0.0 0 0.000 0
1.20 0 0 49238 0.0% -99.9% -99.9% 0 -99.00 -99.9% 0.0 0 0.000 0
1.10 0 0 68746 0.0% -99.9% -99.9% 0 -99.00 -99.9% 0.0 0 0.000 0
1.00 0 0 98884 0.0% -99.9% -99.9% 0 -99.00 -99.9% 0.0 0 0.000 0
0.90 0 0 147505 0.0% -99.9% -99.9% 0 -99.00 -99.9% 0.0 0 0.000 0
0.80 0 0 230396 0.0% -99.9% -99.9% 0 -99.00 -99.9% 0.0 0 0.000 0
total 1579771 119964 778303 15.4% 12.8% 13.1% 1579647 14.33 13.4% 99.9* -1 0.755 111306
========== STATISTICS OF INPUT DATA SET ==========
R-FACTORS FOR INTENSITIES OF DATA SET /dls/sci-scratch/Sam/FC59251/fr6_1/XDS_ASCII.HKL
RESOLUTION R-FACTOR R-FACTOR COMPARED
LIMIT observed expected
20.00 2.7% 3.0% 557
10.00 2.4% 3.1% 5018
6.00 2.8% 3.3% 18351
4.00 3.2% 3.5% 59690
3.00 4.4% 4.4% 112102
2.50 8.7% 8.6% 147954
2.00 21.4% 21.6% 332949
1.90 56.5% 57.1% 106645
1.80 86.8% 87.0% 138516
1.70 140.0% 140.1% 175116
1.60 206.1% 208.5% 209397
1.50 333.4% 342.1% 273340
1.40 42.6% 112.7% 12
1.30 -99.9% -99.9% 0
1.20 -99.9% -99.9% 0
1.10 -99.9% -99.9% 0
1.00 -99.9% -99.9% 0
0.90 -99.9% -99.9% 0
0.80 -99.9% -99.9% 0
total 12.8% 13.1% 1579647
******************************************************************************
WILSON STATISTICS OF SCALED DATA SET: fae-ip.ahkl
******************************************************************************
Data is divided into resolution shells and a straight line
A - 2*B*SS is fitted to log<I>, where
RES = mean resolution (Angstrom) in shell
SS = mean of (sin(THETA)/LAMBDA)**2 in shell
<I> = mean reflection intensity in shell
BO = (A - log<I>)/(2*SS)
# = number of reflections in resolution shell
WILSON LINE (using all data) : A= 14.997 B= 29.252 CORRELATION= 0.99
# RES SS <I> log(<I>) BO
1667 8.445 0.004 2.3084E+06 14.652 49.2
2798 5.260 0.009 1.5365E+06 14.245 41.6
3547 4.106 0.015 2.0110E+06 14.514 16.3
4147 3.480 0.021 1.2910E+06 14.071 22.4
4688 3.073 0.026 7.3586E+05 13.509 28.1
5154 2.781 0.032 4.6124E+05 13.042 30.3
5568 2.560 0.038 3.1507E+05 12.661 30.6
5966 2.384 0.044 2.4858E+05 12.424 29.2
6324 2.240 0.050 1.8968E+05 12.153 28.5
6707 2.119 0.056 1.3930E+05 11.844 28.3
7030 2.016 0.062 9.1378E+04 11.423 29.0
7331 1.926 0.067 5.4413E+04 10.904 30.4
7664 1.848 0.073 3.5484E+04 10.477 30.9
7934 1.778 0.079 2.4332E+04 10.100 31.0
8193 1.716 0.085 1.8373E+04 9.819 30.5
8466 1.660 0.091 1.4992E+04 9.615 29.7
8743 1.609 0.097 1.1894E+04 9.384 29.1
9037 1.562 0.102 9.4284E+03 9.151 28.5
9001 1.520 0.108 8.3217E+03 9.027 27.6
HIGHER ORDER MOMENTS OF WILSON DISTRIBUTION OF CENTRIC DATA
AS COMPARED WITH THEORETICAL VALUES. (EXPECTED: 1.00)
# RES <I**2>/ <I**3>/ <I**4>/
3<I>**2 15<I>**3 105<I>**4
440 8.445 0.740 0.505 0.294
442 5.260 0.762 0.733 0.735
442 4.106 0.888 0.788 0.717
439 3.480 1.339 1.733 2.278
438 3.073 1.168 1.259 1.400
440 2.781 1.215 1.681 2.269
438 2.560 1.192 1.603 2.405
450 2.384 1.117 1.031 0.891
432 2.240 1.214 1.567 2.173
438 2.119 0.972 0.992 0.933
445 2.016 1.029 1.019 0.986
441 1.926 1.603 1.701 1.554
440 1.848 1.544 1.871 2.076
436 1.778 0.927 0.661 0.435
444 1.716 1.134 1.115 1.197
440 1.660 1.271 1.618 2.890
436 1.609 1.424 1.045 0.941
448 1.562 1.794 1.447 1.423
426 1.520 2.517 1.496 2.099
8355 overall 1.253 1.255 1.455
HIGHER ORDER MOMENTS OF WILSON DISTRIBUTION OF ACENTRIC DATA
AS COMPARED WITH THEORETICAL VALUES. (EXPECTED: 1.00)
# RES <I**2>/ <I**3>/ <I**4>/
2<I>**2 6<I>**3 24<I>**4
1227 8.445 1.322 1.803 2.340
2356 5.260 1.167 1.420 1.789
3105 4.106 1.010 1.046 1.100
3708 3.480 1.055 1.262 1.592
4250 3.073 0.999 1.083 1.375
4714 2.781 1.061 1.232 1.591
5130 2.560 1.049 1.178 1.440
5516 2.384 1.025 1.117 1.290
5892 2.240 1.001 1.058 1.230
6269 2.119 1.060 1.140 1.233
6585 2.016 1.109 1.344 1.709
6890 1.926 1.028 1.100 1.222
7224 1.848 1.060 1.150 1.348
7498 1.778 1.143 1.309 1.655
7749 1.716 1.182 1.299 1.549
8026 1.660 1.286 1.376 1.538
8307 1.609 1.419 1.481 1.707
8589 1.562 1.663 1.750 2.119
8575 1.520 2.271 2.172 5.088
111610 overall 1.253 1.354 1.804
======= CUMULATIVE INTENSITY DISTRIBUTION =======
DEFINITIONS:
<I> = mean reflection intensity
Na(Z)exp = expected number of acentric reflections with I <= Z*<I>
Na(Z)obs = observed number of acentric reflections with I <= Z*<I>
Nc(Z)exp = expected number of centric reflections with I <= Z*<I>
Nc(Z)obs = observed number of centric reflections with I <= Z*<I>
Nc(Z)obs/Nc(Z)exp versus resolution and Z (0.1-1.0)
# RES 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
440 8.445 0.75 0.95 0.98 1.00 0.98 0.99 1.00 1.00 1.02 1.02
442 5.260 1.18 1.11 1.09 1.09 1.07 1.08 1.08 1.08 1.07 1.06
442 4.106 0.97 1.01 0.98 0.97 0.96 0.94 0.92 0.91 0.92 0.94
439 3.480 0.91 0.88 0.91 0.91 0.89 0.90 0.90 0.89 0.89 0.93
438 3.073 0.92 0.92 0.90 0.93 0.94 0.99 1.02 0.99 0.96 0.96
440 2.781 0.98 1.01 1.02 1.05 1.04 1.03 1.04 1.02 1.01 1.01
438 2.560 1.02 1.10 1.05 1.03 1.01 1.03 1.04 1.01 1.04 1.02
450 2.384 0.78 0.93 0.92 0.93 0.89 0.89 0.92 0.95 0.96 0.95
432 2.240 0.69 0.82 0.84 0.86 0.91 0.92 0.93 0.94 0.95 0.95
438 2.119 0.75 0.87 0.95 1.02 1.09 1.09 1.12 1.12 1.10 1.08
445 2.016 0.86 0.86 0.87 0.90 0.91 0.93 0.98 0.99 1.00 1.00
441 1.926 0.88 0.79 0.79 0.81 0.82 0.84 0.85 0.85 0.86 0.86
440 1.848 1.00 0.89 0.85 0.83 0.85 0.85 0.88 0.90 0.90 0.92
436 1.778 1.03 0.87 0.79 0.79 0.80 0.84 0.85 0.87 0.90 0.92
444 1.716 1.09 0.85 0.81 0.78 0.80 0.80 0.81 0.81 0.84 0.85
440 1.660 1.27 1.01 0.93 0.88 0.85 0.84 0.84 0.85 0.88 0.91
436 1.609 1.34 1.00 0.89 0.83 0.80 0.80 0.80 0.81 0.80 0.83
448 1.562 1.39 1.09 0.93 0.86 0.81 0.78 0.77 0.79 0.78 0.78
426 1.520 1.38 1.03 0.88 0.83 0.82 0.80 0.78 0.76 0.75 0.74
8355 overall 1.01 0.95 0.92 0.91 0.91 0.91 0.92 0.92 0.93 0.93
Na(Z)obs/Na(Z)exp versus resolution and Z (0.1-1.0)
# RES 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
1227 8.445 1.10 1.22 1.21 1.21 1.14 1.10 1.12 1.10 1.11 1.09
2356 5.260 1.15 1.10 1.09 1.03 1.03 1.03 1.01 1.01 1.01 1.00
3105 4.106 0.91 0.96 0.99 1.01 1.02 1.00 1.00 0.99 0.99 1.00
3708 3.480 0.93 0.97 1.00 1.06 1.05 1.04 1.04 1.04 1.04 1.05
4250 3.073 0.94 1.02 1.01 1.00 1.01 1.00 1.00 1.01 1.02 1.02
4714 2.781 1.11 1.04 1.02 1.02 1.02 1.01 1.01 1.01 1.00 1.00
5130 2.560 1.00 1.10 1.06 1.03 1.01 1.02 1.01 1.01 1.01 1.02
5516 2.384 1.09 1.08 1.05 1.04 1.04 1.02 1.01 1.01 1.01 1.01
5892 2.240 0.98 0.99 1.00 1.01 1.01 1.01 1.00 1.00 1.00 1.00
6269 2.119 1.14 1.04 1.02 1.00 1.00 1.00 1.01 1.02 1.02 1.01
6585 2.016 1.17 1.02 1.01 1.02 1.02 1.03 1.02 1.02 1.02 1.02
6890 1.926 1.35 1.07 1.00 0.99 1.00 1.01 1.01 1.00 1.00 1.01
7224 1.848 1.52 1.11 1.01 0.97 0.96 0.98 0.98 0.98 0.98 0.99
7498 1.778 1.80 1.22 1.03 0.97 0.95 0.94 0.95 0.95 0.95 0.96
7749 1.716 2.01 1.28 1.07 0.99 0.94 0.92 0.92 0.92 0.93 0.93
8026 1.660 2.31 1.41 1.13 1.01 0.95 0.92 0.90 0.89 0.89 0.89
8307 1.609 2.62 1.54 1.19 1.04 0.95 0.90 0.88 0.87 0.86 0.87
8589 1.562 2.94 1.69 1.29 1.10 1.00 0.93 0.89 0.86 0.85 0.85
8575 1.520 3.14 1.78 1.34 1.13 1.01 0.93 0.88 0.85 0.83 0.83
111610 overall 1.73 1.24 1.09 1.03 0.99 0.97 0.96 0.96 0.96 0.96
List of 33 reflections *NOT* obeying Wilson distribution (Z> 10.0)
h k l RES Z Intensity Sigma
72 11 61 1.52 17.34 0.2886E+06 0.2367E+05 "alien"
67 53 6 1.50 15.85 0.2638E+06 0.1128E+06 "alien"
35 10 25 3.17 14.39 0.2118E+08 0.2364E+06 "alien"
46 17 99 1.50 14.16 0.2357E+06 0.9588E+05 "alien"
34 32 2 2.75 13.44 0.1239E+08 0.1279E+06 "alien"
79 6 15 1.60 13.10 0.3117E+06 0.2477E+05 "alien"
61 20 33 1.88 12.54 0.8900E+06 0.3054E+05 "alien"
44 4 48 2.30 12.38 0.4695E+07 0.6072E+05 "alien"
66 25 19 1.79 11.89 0.5788E+06 0.2739E+05 "alien"
66 25 11 1.81 11.88 0.5781E+06 0.2771E+05 "alien"
60 43 61 1.50 11.77 0.1959E+06 0.9769E+05 "alien"
72 11 17 1.74 11.64 0.4278E+06 0.2619E+05 "alien"
80 24 26 1.50 11.41 0.1899E+06 0.9793E+05 "alien"
41 21 26 2.59 11.09 0.6988E+07 0.7945E+05 "alien"
44 18 20 2.59 11.08 0.6982E+07 0.7839E+05 "alien"
23 3 62 2.59 11.06 0.6971E+07 0.9154E+05 "alien"
69 7 22 1.80 11.06 0.5383E+06 0.2564E+05 "alien"
73 10 15 1.72 10.98 0.4036E+06 0.2356E+05 "alien"
70 17 35 1.68 10.96 0.3286E+06 0.2415E+05 "alien"
57 24 41 1.88 10.91 0.7746E+06 0.2842E+05 "alien"
82 24 6 1.50 10.74 0.1787E+06 0.1019E+06 "alien"
69 25 62 1.50 10.67 0.1775E+06 0.8689E+05 "alien"
24 20 44 2.91 10.45 0.9641E+07 0.1017E+06 "alien"
66 43 5 1.63 10.37 0.2468E+06 0.2294E+05 "alien"
81 4 29 1.53 10.36 0.1725E+06 0.2364E+05 "alien"
60 40 26 1.72 10.32 0.3792E+06 0.2578E+05 "alien"
39 18 57 2.18 10.24 0.3885E+07 0.5573E+05 "alien"
70 41 15 1.57 10.19 0.1922E+06 0.2281E+05 "alien"
55 36 41 1.79 10.16 0.4942E+06 0.2967E+05 "alien"
37 4 81 1.88 10.15 0.7202E+06 0.3357E+05 "alien"
56 27 5 2.06 10.14 0.1854E+07 0.3569E+05 "alien"
44 39 29 2.06 10.09 0.1844E+07 0.3805E+05 "alien"
65 46 29 1.56 10.06 0.1898E+06 0.2270E+05 "alien"
List of 33 reflections *NOT* obeying Wilson distribution (sorted by resolution)
Ice rings could occur at (Angstrom):
3.897,3.669,3.441, 2.671,2.249,2.072, 1.948,1.918,1.883,1.721
h k l RES Z Intensity Sigma
82 24 6 1.50 10.74 0.1787E+06 0.1019E+06
67 53 6 1.50 15.85 0.2638E+06 0.1128E+06
80 24 26 1.50 11.41 0.1899E+06 0.9793E+05
60 43 61 1.50 11.77 0.1959E+06 0.9769E+05
69 25 62 1.50 10.67 0.1775E+06 0.8689E+05
46 17 99 1.50 14.16 0.2357E+06 0.9588E+05
72 11 61 1.52 17.34 0.2886E+06 0.2367E+05
81 4 29 1.53 10.36 0.1725E+06 0.2364E+05
65 46 29 1.56 10.06 0.1898E+06 0.2270E+05
70 41 15 1.57 10.19 0.1922E+06 0.2281E+05
79 6 15 1.60 13.10 0.3117E+06 0.2477E+05
66 43 5 1.63 10.37 0.2468E+06 0.2294E+05
70 17 35 1.68 10.96 0.3286E+06 0.2415E+05
73 10 15 1.72 10.98 0.4036E+06 0.2356E+05
60 40 26 1.72 10.32 0.3792E+06 0.2578E+05
72 11 17 1.74 11.64 0.4278E+06 0.2619E+05
66 25 19 1.79 11.89 0.5788E+06 0.2739E+05
55 36 41 1.79 10.16 0.4942E+06 0.2967E+05
69 7 22 1.80 11.06 0.5383E+06 0.2564E+05
66 25 11 1.81 11.88 0.5781E+06 0.2771E+05
61 20 33 1.88 12.54 0.8900E+06 0.3054E+05
57 24 41 1.88 10.91 0.7746E+06 0.2842E+05
37 4 81 1.88 10.15 0.7202E+06 0.3357E+05
56 27 5 2.06 10.14 0.1854E+07 0.3569E+05
44 39 29 2.06 10.09 0.1844E+07 0.3805E+05
39 18 57 2.18 10.24 0.3885E+07 0.5573E+05
44 4 48 2.30 12.38 0.4695E+07 0.6072E+05
44 18 20 2.59 11.08 0.6982E+07 0.7839E+05
41 21 26 2.59 11.09 0.6988E+07 0.7945E+05
23 3 62 2.59 11.06 0.6971E+07 0.9154E+05
34 32 2 2.75 13.44 0.1239E+08 0.1279E+06
24 20 44 2.91 10.45 0.9641E+07 0.1017E+06
35 10 25 3.17 14.39 0.2118E+08 0.2364E+06
cpu time used by XSCALE 25.9 sec
elapsed wall-clock time 28.1 sec
I would like to extract the second last line where the 11th column has a number followed by an asterisk (xy.z*) and the lines above and below that. 我想提取第二行的第二行，其中第11列有一个数字后跟一个星号（xy.z *）以及上面和下面的行。 That is from the table with SUBSET OF INTENSITY DATA WITH SIGNAL/NOISE >= -3.0 AS FUNCTION OF RESOLUTION Above it. 这是从具有信号/噪声> = -3.0的强度子集的表作为其上面的分辨率的函数。
For example in this table the line I'm looking for would contain "23.2*" from the 11th column (CC(1/2)). 例如，在该表中，我正在寻找的行将包含来自第11列（CC（1/2））的“23.2 *”。 I would like the second last with an asterisk because the last would be the line that starts with total, and this was a lot easier to extract with a simple grep command. 我希望倒数第二个带星号，因为最后一个是以total开头的行，并且使用简单的grep命令提取起来要容易得多。
So the expected output for the code in this case would be to print the lines: 因此，在这种情况下代码的预期输出将是打印行：
1.60 209398 16298 16304 100.0% 206.1% 208.5% 209397 1.35 214.6% 48.9* -2 0.693 15466
1.50 273432 20770 20893 99.4% 333.4% 342.1% 273340 0.80 346.9% 23.2* -1 0.644 19495
1.40 33 27 27248 0.1% 42.6% 112.7% 12 0.40 60.3% 88.2 0 0.000 0
And so on for all the different possible positions of the asterisk in the table. 等等表格中星号的所有不同位置。
In my previous question I recieved the answer 在我之前的问题中，我收到了答案
sed -n '/LIMIT/,/=/{/^\s*\(\S*\s*\)\{10\}[0-9.-]*\*/H;x;s/^.*\n\(.*\n.*\)$/\1/;x;/=/{x;P;q}}' file
Which worked really well (thanks Endoro) for extracting just the second last line in the 11th column with the asterisk, (which is what i asked for) but now I just need that editing slightly, or if you would rather make a whole new line, to include the lines above and below. 哪个工作得非常好（感谢Endoro）用星号提取第11列中的第二行（这就是我要求的）但是现在我只需稍微编辑一下，或者如果你想要创建一个全新的行，包括上面和下面的线。
Here is a link to the previous question Extracting the second last line from a table using a specific number followed by an asterisk (eg xy.z*) 以下是上一个问题的链接使用特定数字后跟星号（例如xy.z *）从表中提取第二个最后一行
Any help would be greatly appreciated. 任何帮助将不胜感激。
Sam 山姆
2 个解决方案
解决方案1
3 已采纳 2013-07-02 21:04:30
sed -rn '/LIMIT/,/total/{//!H};/total/{x;s/^.*\n(.*\n)((\s+\S+){10}\s+[0-9.]+\*(\s+\S+){3}\n(\s+\S+){14}).*/\1\2/;p;q}' file
$sed -rn '/LIMIT/,/total/{//!H};/total/{x;s/^.*\n(.*\n)((\s+\S+){10}\s+[0-9.]+\*(\s+\S+){3}\n(\s+\S+){14}).*/\1\2/;p;q}' file
1.60 209398 16298 16304 100.0% 206.1% 208.5% 209397 1.35 214.6% 48.9* -2 0.693 15466
1.50 273432 20770 20893 99.4% 333.4% 342.1% 273340 0.80 346.9% 23.2* -1 0.644 19495
1.40 33 27 27248 0.1% 42.6% 112.7% 12 0.40 60.3% 88.2 0 0.000 0
解决方案2
1 2013-07-02 15:35:02
A bit dirty but should work: 有点脏，但应该工作：
awk '
/^ *SUBSET OF INTENSITY/,/^ *total/ {
a[++i]=$0;
b[i]=$11
}
END {
for(o=i-1;o>=0;o--)
if (b[o]~/\*/) {
print a[o-1]"\n"a[o]"\n"a[o+1]
break
}
}' log
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