从日志文件中提取数据的特定行 [英] Extracting specific lines of data from a log file
本文介绍了从日志文件中提取数据的特定行的处理方法，对大家解决问题具有一定的参考价值，需要的朋友们下面随着小编来一起学习吧！
问题描述
我期待提取和打印从表中我有一个很长的日志文件中的特定行。它看起来是这样的：
I'm looking to extract and print a specific line from a table I have in a long log file. It looks something like this:
******************************************************************************
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
我想提取倒数第二行，其中第11列在数字后面跟着星号（* xy.z）和上面和下面的行。这是从子集的信号/噪声强度数据> = -3.0 AS函数解析它上面的表中。
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. That is from the table with SUBSET OF INTENSITY DATA WITH SIGNAL/NOISE >= -3.0 AS FUNCTION OF RESOLUTION Above it.
例如本表我在寻找将包含* 23.2从第11列线（CC（1/2））。我想的倒数第二个有星号，因为最后的将是总开头的行，这是一个更容易用一个简单的grep命令来提取。
For example in this table the line I'm looking for would contain "23.2*" from the 11th column (CC(1/2)). 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.
因此，在这种情况下，期望的输出为code将打印行：
So the expected output for the code in this case would be to print the lines:
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
和等在表中的星号的所有不同的可能位置。
And so on for all the different possible positions of the asterisk in the table.
在我的previous的问题，我收到的答案
In my previous question I recieved the answer
sed -n '/LIMIT/,/=/{/^\s*\(\S*\s*\)\{10\}[0-9.-]*\*/H;x;s/^.*\n\(.*\n.*\)$/\1/;x;/=/{x;P;q}}' file
这对于提取正好与星号的第11列倒数第二行确实行之有效（感谢Endoro），（这是我要的是），但现在我只需要一个编辑咯，或者如果你宁愿做一个全新的线，包括上面和下面的行。
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.
下面是对previous问题<一个链接href=\"http://stackoverflow.com/questions/16936606/extracting-the-second-last-line-from-a-table-using-a-specific-number-followed-by\">Extracting从表中使用特定数量的倒数第二行，后跟一个星号（例如* xy.z）
Here is a link to the previous question Extracting the second last line from a table using a specific number followed by an asterisk (e.g. xy.z*)
任何帮助将大大AP preciated。
Any help would be greatly appreciated.
山姆
推荐答案
$ C $为GNU的 SED
Code for GNU sed
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
这篇关于从日志文件中提取数据的特定行的文章就介绍到这了，希望我们推荐的答案对大家有所帮助，也希望大家多多支持IT屋！
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