This repository was archived by the owner on Jan 25, 2023. It is now read-only.
-
Notifications
You must be signed in to change notification settings - Fork 1
Expand file tree
/
Copy pathinternal_origin_script.py
More file actions
588 lines (516 loc) · 25 KB
/
internal_origin_script.py
File metadata and controls
588 lines (516 loc) · 25 KB
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
208
209
210
211
212
213
214
215
216
217
218
219
220
221
222
223
224
225
226
227
228
229
230
231
232
233
234
235
236
237
238
239
240
241
242
243
244
245
246
247
248
249
250
251
252
253
254
255
256
257
258
259
260
261
262
263
264
265
266
267
268
269
270
271
272
273
274
275
276
277
278
279
280
281
282
283
284
285
286
287
288
289
290
291
292
293
294
295
296
297
298
299
300
301
302
303
304
305
306
307
308
309
310
311
312
313
314
315
316
317
318
319
320
321
322
323
324
325
326
327
328
329
330
331
332
333
334
335
336
337
338
339
340
341
342
343
344
345
346
347
348
349
350
351
352
353
354
355
356
357
358
359
360
361
362
363
364
365
366
367
368
369
370
371
372
373
374
375
376
377
378
379
380
381
382
383
384
385
386
387
388
389
390
391
392
393
394
395
396
397
398
399
400
401
402
403
404
405
406
407
408
409
410
411
412
413
414
415
416
417
418
419
420
421
422
423
424
425
426
427
428
429
430
431
432
433
434
435
436
437
438
439
440
441
442
443
444
445
446
447
448
449
450
451
452
453
454
455
456
457
458
459
460
461
462
463
464
465
466
467
468
469
470
471
472
473
474
475
476
477
478
479
480
481
482
483
484
485
486
487
488
489
490
491
492
493
494
495
496
497
498
499
500
501
502
503
504
505
506
507
508
509
510
511
512
513
514
515
516
517
518
519
520
521
522
523
524
525
526
527
528
529
530
531
532
533
534
535
536
537
538
539
540
541
542
543
544
545
546
547
548
549
550
551
552
553
554
555
556
557
558
559
560
561
562
563
564
565
566
567
568
569
570
571
572
573
574
575
576
577
578
579
580
581
582
583
584
585
586
587
588
# -*- coding: utf-8 -*-
"""
This is the internal Origin python script which runs inside Origin when
Origin is called externally from python.
Created on Thu Mar 7 15:01:32 2019
@author: ericmuckley@gmail.com
"""
import PyOrigin
import os
import sys
import csv
import glob
# add path to non-standard python libraries so they can be imported
# lib_path = 'C:\\ProgramData\\Anaconda3\\Lib\\site-packages'
# sys.path.append(lib_path)
# these imports will only work if pandas is installed in Origin first!
import numpy as np
import pandas as pd
def import_csv(filename):
# imports a csv file and returns headers and data as floats
data = []
with open(filename) as f:
reader = csv.reader(f)
[data.append(row) for row in reader]
# extact headers
headers = data[0]
# remove headers from data
data = data[1:]
# convert strings to floats
for i in range(len(data)):
for j in range(len(data[i])):
if data[i][j] == '':
data[i][j] = '0'
data[i][j] = float(data[i][j])
# remove completely empty rows from data
data = [row for row in data if not all(i == 0 for i in row)]
# transpose data
data = list(map(list, zip(*data)))
return headers, data
def get_file_dict(exp_start_time, data_folder):
# get a dictionary of each data file and what type of data it holds based
# on the experiment start time and folder of data files.
# get list of all data files in data folder
all_data_files = glob.glob(data_folder + '\*')
# list of data descriptors (strings) which should show up in file names
data_file_descriptors = ['main_df', 'qcm_params', 'iv', 'cv', 'eis',
'bs', 'optical']
# create empty dictionary to hold selected data files
file_dict = {}
# loop through all data files in the data folder
for f in all_data_files:
# split full file path into file directory and name
filedir, filename = os.path.split(f)
# get date of file creation from beginning of filename
filedate = filename.split('__')[0]
# select files which creation date matches that of exp_start_time
if filedate == exp_start_time:
# assign each datafile to each file descriptor
for descriptor in data_file_descriptors:
if descriptor in filename:
file_dict[descriptor] = f
return file_dict
def norm_qcm_params(data):
# get arrays of normalized QCM parameters from delta F and delta D data.
# input should be values of the raw data from qcm_params.csv:
# i.e. pd.read_csv('qcm_params.csv).values
# the normalized data is raw data minus original baseline divided by n.
# separate deltaF from deltaD columns
df_raw = data[:, 0:10]
dd_raw = data[:, [0, 10, 11, 12, 13, 14, 15, 16, 17, 18]]
# create copy arrays for normalized data
df_norm = np.copy(df_raw)
dd_norm = np.copy(dd_raw)
# loop over each column of raw data
for col in range(1, len(df_raw[0])):
# get harmonic number
n = (col - 1) * 2 + 1
# find indicies which have data in them
data_indices = np.invert(np.isnan(df_raw[:, col]))
# check if there is any data in the column
if len(data_indices) > 0:
# index to normalize column on (the 1st measurement in the column)
norm_index = np.argmax(data_indices)
# get delta f/n and delta D/n
df_norm[data_indices, col] = (
df_raw[data_indices, col] - df_raw[norm_index, col])/n/1e3
dd_norm[data_indices, col] = (
dd_raw[data_indices, col] - dd_raw[norm_index, col]) / 1e-6
return df_norm, dd_norm
def get_sheet(file, data):
# get Origin worksheet and fill it with data
# create workbook named 'file' using template named 'Origin'
PyOrigin.CreatePage(PyOrigin.PGTYPE_WKS, file, 'Origin', 1)
sheet = PyOrigin.ActiveLayer() # get sheet
sheet.SetData(data.T, -1) # put imported data into worksheet
sheet.SetName(file) # set sheet name
return sheet
def get_plot(file, template='custom_line'):
# create empty origin plot to fill with data using specified template
pgName = PyOrigin.CreatePage(
PyOrigin.PGTYPE_GRAPH,
'plot_'+file, template, 1)
gp = PyOrigin.Pages(str(pgName))
gp.LT_execute('layer1.x.opposite = 1;layer1.y.opposite = 1;')
gp.LT_execute('layer1 -g')
gl = gp.Layers(0)
# Create data range and plot it into the graph layer.
rng = PyOrigin.NewDataRange() # Create data range.
return gl, rng
# get path of data folder
exp_start_time = sys.argv[1]
exp_start_time = exp_start_time[:-1] # remove trailing underscore
data_folder = sys.argv[2]
# get list of relevant data files
file_dict = get_file_dict(exp_start_time, data_folder)
# save origin file and quit
save_origin_filename = os.path.join(
data_folder,
exp_start_time+'_origin_report.opj')
# loop over every relevant data file and open new worksheet for each one
for file in file_dict:
# if there is data, import data files
if file_dict:
data = pd.read_csv(file_dict[file]).values
headers = list(pd.read_csv(file_dict[file]))
if file == 'main_df':
# re-read data as dataframe, not values
data = pd.read_csv(file_dict[file])
# cut off last values
data = data.iloc[:-10]
# create elapsed time column
elapsed_time = (np.array(data['time']) - data['time'].iloc[0])/60
# insert elapsed time column into dataframe
data.insert(loc=2, column='Time', value=elapsed_time)
# create worksheet and plot
sheet = get_sheet(file, data.values)
# loop over columns and label them
for col in range(len(data)):
if list(data)[col] == 'date':
sheet.Columns(col).SetLongName('Date/time')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_X)
if list(data)[col] == 'time':
sheet.Columns(col).SetLongName('Time')
sheet.Columns(col).SetUnits('min')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_X)
if list(data)[col] == 'Time':
sheet.Columns(col).SetLongName('Time')
sheet.Columns(col).SetUnits('hours')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_X)
if list(data)[col] == 'pressure':
sheet.Columns(col).SetLongName('pressure_measured')
sheet.Columns(col).SetUnits('Torr')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'pressure_setpoint':
sheet.Columns(col).SetLongName('Pressure')
sheet.Columns(col).SetUnits('Torr')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'mfc1':
sheet.Columns(col).SetLongName('Flow-1')
sheet.Columns(col).SetUnits('SCCM')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'mfc2':
sheet.Columns(col).SetLongName('Flow-2')
sheet.Columns(col).SetUnits('SCCM')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'rh':
sheet.Columns(col).SetLongName('rh_measured')
sheet.Columns(col).SetUnits('%')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'rh_setpoint':
sheet.Columns(col).SetLongName('RH')
sheet.Columns(col).SetUnits('%')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'temp':
sheet.Columns(col).SetLongName('Temperature')
sheet.Columns(col).SetUnits('C')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'bias':
sheet.Columns(col).SetLongName('Bias')
sheet.Columns(col).SetUnits('V')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'current':
sheet.Columns(col).SetLongName('Current')
sheet.Columns(col).SetUnits('A')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'max_iv_current':
sheet.Columns(col).SetLongName('Max. I-V current')
sheet.Columns(col).SetUnits('A')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'max_cv_current':
sheet.Columns(col).SetLongName('Max. C-V current')
sheet.Columns(col).SetUnits('A')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'cv_area':
sheet.Columns(col).SetLongName('C-V area')
sheet.Columns(col).SetUnits('V x A')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'low_freq_z':
sheet.Columns(col).SetLongName('Low freq. Z')
sheet.Columns(col).SetUnits('Ohm')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
if list(data)[col] == 'note':
sheet.Columns(col).SetLongName('Note')
sheet.Columns(col).SetType(PyOrigin.COLTYPE_DESIGN_Y)
try:
# plot RH during experiment
gl, rng = get_plot(file+'_rh')
rng.Add('X', sheet, 0, data.columns.get_loc('Time'),
-1, data.columns.get_loc('Time'))
rng.Add('Y', sheet, 0, data.columns.get_loc('RH'),
-1, data.columns.get_loc('RH'))
dp = gl.AddPlot(rng, 200)
# plot pressure during experiment
gl, rng = get_plot(file+'_rh')
rng.Add('X', sheet, 0, data.columns.get_loc('Time'),
-1, data.columns.get_loc('Time'))
rng.Add('Y', sheet, 0, data.columns.get_loc('Pressure'),
-1, data.columns.get_loc('Pressure'))
dp = gl.AddPlot(rng, 200)
except:
pass
if file == 'iv':
# change units
for i in range(0, len(data[0]), 2):
data[:, i+1] = data[:, i+1] * 1e9
# create worksheet and plot
sheet = get_sheet(file, data)
gl, rng = get_plot(file)
for i in range(0, len(data[0]), 2):
sheet.Columns(i).SetLongName('Bias')
sheet.Columns(i).SetUnits('V')
sheet.Columns(i).SetComments(str(1+int(i/2)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Current')
sheet.Columns(i+1).SetUnits('nA')
sheet.Columns(i+1).SetComments(str(1+int(i/2)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+1 col as Y
rng.Add('Y', sheet, 0, i+1, -1, i+1)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
elif file == 'cv':
# change units and cut off redundant cycles
# cycle_length = int((len(data) - 1)/4)
# data = data[cycle_length-1:-cycle_length]
# for i in range(0, len(data[0]), 2):
# data[:, i+1] = data[:, i+1] * 1e9
# create worksheet and plot
sheet = get_sheet(file, data)
gl, rng = get_plot(file)
for i in range(0, len(data[0]), 2):
if 'bias' in headers[i]:
pass
sheet.Columns(i).SetLongName('Bias')
sheet.Columns(i).SetUnits('V')
sheet.Columns(i).SetComments(str(1+int(i/2)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Current')
sheet.Columns(i+1).SetUnits('A')
sheet.Columns(i+1).SetComments(str(1+int(i/2)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+1 col as Y
rng.Add('Y', sheet, 0, i+1, -1, i+1)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
elif file == 'bs':
# change units
for i in range(0, len(data[0]), 3):
data[:, i+2] = data[:, i+2] * 1e9
# create worksheet and plot
sheet = get_sheet(file, data)
gl, rng = get_plot(file)
for i in range(0, len(data[0]), 3):
sheet.Columns(i).SetLongName('Time')
sheet.Columns(i).SetUnits('min')
sheet.Columns(i).SetComments(str(1+int(i/3)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Bias')
sheet.Columns(i+1).SetUnits('V')
sheet.Columns(i+1).SetComments(str(1+int(i/3)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
sheet.Columns(i+2).SetUnits('nA')
sheet.Columns(i+2).SetLongName('Current')
sheet.Columns(i+2).SetComments(str(1+int(i/3)))
sheet.Columns(i+2).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -10, i)
# graph worksheet's i+2 col as Y
rng.Add('Y', sheet, 0, i+2, -10, i+2)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
elif file == 'optical':
# create worksheet and plot
sheet = get_sheet(file, data)
gl, rng = get_plot(file)
for i in range(0, len(data[0]), 2):
sheet.Columns(i).SetLongName('Wavelength')
sheet.Columns(i).SetUnits('nm')
sheet.Columns(i).SetComments(str(1+int(i/2)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Intensity')
sheet.Columns(i+1).SetUnits('counts')
sheet.Columns(i+1).SetComments(str(1+int(i/2)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+2 col as Y
rng.Add('Y', sheet, 0, i+1, -1, i+1)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
elif file == 'eis':
# only select data columns corresponding to Bode Z data
data_bd_z = np.empty((len(data), 0))
for i in range(0, len(data[0]), 5):
data_bd_z = np.column_stack((data_bd_z, data[:, i]))
data_bd_z = np.column_stack((data_bd_z, data[:, i+1]/1e6))
# create worksheet and plot
sheet = get_sheet(file+'_bode_z', data_bd_z)
# create impedance plot
gl, rng = get_plot(file+'_z')
for i in range(0, len(data_bd_z[0]), 2):
sheet.Columns(i).SetLongName('Frequency')
sheet.Columns(i).SetUnits('Hz')
sheet.Columns(i).SetComments(str(1+int(i/2)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Z')
sheet.Columns(i+1).SetUnits('MOhm')
sheet.Columns(i+1).SetComments(str(1+int(i/2)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+1 col as Y
rng.Add('Y', sheet, 0, i+1, -1, i+1)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
# Z data with only one frequency column for heatmap plotting
# use the last set of measured frequencies as "X" column
data_bd_z2 = data[:, -5]
for i in range(0, len(data[0]), 5):
data_bd_z2 = np.column_stack((data_bd_z2, data[:, i+1]/1e6))
# create worksheet and plot
sheet = get_sheet('bode_z_clean', data_bd_z2)
# create plot
# gl, rng = get_plot('z_clean')
sheet.Columns(0).SetLongName('Frequency')
sheet.Columns(0).SetUnits('Hz')
sheet.Columns(0).SetComments('0')
sheet.Columns(0).SetType(PyOrigin.COLTYPE_DESIGN_X)
# rng.Add('X', sheet, 0, 0, -1, 0)
for i in range(1, len(data_bd_z2[0])):
sheet.Columns(i).SetLongName('Z')
sheet.Columns(i).SetUnits('MOhm')
sheet.Columns(i).SetComments(str(i-1))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's Y columns
# rng.Add('Y', sheet, 0, i, -1, i)
# dp = gl.AddPlot(rng, 200)
# PyOrigin.LT_execute('layer -g')
# only select data columns corresponding to Bode phase data
data_bd_phi = np.empty((len(data), 0))
for i in range(0, len(data[0]), 5):
data_bd_phi = np.column_stack((data_bd_phi, data[:, i]))
data_bd_phi = np.column_stack((data_bd_phi, data[:, i+2]))
# create worksheet and plot
sheet = get_sheet(file+'_bode_phase', data_bd_phi)
# create phase plot
gl, rng = get_plot(file+'_phase')
for i in range(0, len(data_bd_phi[0]), 2):
sheet.Columns(i).SetLongName('Frequency')
sheet.Columns(i).SetUnits('Hz')
sheet.Columns(i).SetComments(str(1+int(i/2)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Phase')
sheet.Columns(i+1).SetUnits('deg')
sheet.Columns(i+1).SetComments(str(1+int(i/2)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+1 col as Y
rng.Add('Y', sheet, 0, i+1, -1, i+1)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
# phase data with only one frequency column for heatmap plotting
# use the last set of measured frequencies as "X" column
data_bd_phi2 = data[:, -5]
for i in range(0, len(data[0]), 5):
data_bd_phi2 = np.column_stack((data_bd_phi2, data[:, i+2]))
# create worksheet and plot
sheet = get_sheet('bode_phase_clean', data_bd_phi2)
# create phase plot
# gl, rng = get_plot('phase_clean')
sheet.Columns(0).SetLongName('Frequency')
sheet.Columns(0).SetUnits('Hz')
sheet.Columns(0).SetComments('0')
sheet.Columns(0).SetType(PyOrigin.COLTYPE_DESIGN_X)
# rng.Add('X', sheet, 0, 0, -1, 0)
for i in range(1, len(data_bd_phi2[0])):
sheet.Columns(i).SetLongName('Phase')
sheet.Columns(i).SetUnits('deg')
sheet.Columns(i).SetComments(str(i-1))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's Y columns
# rng.Add('Y', sheet, 0, i, -1, i)
# dp = gl.AddPlot(rng, 200)
# PyOrigin.LT_execute('layer -g')
# only select data columns corresponding to Nyquist data
data_ny = np.empty((len(data), 0))
for i in range(0, len(data[0]), 5):
data_ny = np.column_stack((data_ny, data[:, i+3]/1e6))
data_ny = np.column_stack((data_ny, data[:, i+4]/1e6))
# create worksheet and plot
sheet = get_sheet(file+'_nyquist', data_ny)
# create impedance plot
gl, rng = get_plot(file+'_nyquist')
for i in range(0, len(data_ny[0]), 2):
sheet.Columns(i).SetLongName('Re(Z)')
sheet.Columns(i).SetUnits('MOhm')
sheet.Columns(i).SetComments(str(1+int(i/2)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Im(Z)')
sheet.Columns(i+1).SetUnits('MOhm')
sheet.Columns(i+1).SetComments(str(1+int(i/2)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+2 col as Y
rng.Add('Y', sheet, 0, i+1, -1, i+1)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
'''
#only select data columns corresponding to Bode data
data_bd = np.empty((len(data), 0))
for i in range(0, len(data[0]), 5):
data_bd = np.column_stack((data_bd, data[:, i]))
data_bd = np.column_stack((data_bd, data[:, i+1]/1e6))
data_bd = np.column_stack((data_bd, data[:, i+2]))
#create worksheet and plot
sheet = get_sheet(file+'_bode', data_bd)
# create impedance plot
gl, rng = get_plot(file+'_z')
for i in range(0, len(data_bd[0]), 3):
sheet.Columns(i).SetLongName('Frequency')
sheet.Columns(i).SetUnits('Hz')
sheet.Columns(i).SetComments(str(1+int(i/3)))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_X)
sheet.Columns(i+1).SetLongName('Z')
sheet.Columns(i+1).SetUnits('MOhm')
sheet.Columns(i+1).SetComments(str(1+int(i/3)))
sheet.Columns(i+1).SetType(PyOrigin.COLTYPE_DESIGN_Y)
sheet.Columns(i+2).SetLongName('Phase')
sheet.Columns(i+2).SetUnits('deg')
sheet.Columns(i+2).SetComments(str(1+int(i/3)))
sheet.Columns(i+2).SetType(PyOrigin.COLTYPE_DESIGN_Y)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+2 col as Y
rng.Add('Y', sheet, 0, i+1, -1, i+1)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
# create phase plot
gl, rng = get_plot(file+'_phase')
for i in range(0, len(data_bd[0]), 5):
# graph worksheet's i col as X
rng.Add('X', sheet, 0, i, -1, i)
# graph worksheet's i+2 col as Y
rng.Add('Y', sheet, 0, i+2, -1, i+2)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
'''
elif file == 'qcm_params':
# separate delta f and delta D data and normalize by n
df_norm, dd_norm = norm_qcm_params(data)
# delta F
# create worksheet and plot
sheet = get_sheet(file+'_df', df_norm)
gl, rng = get_plot(file+'_df')
sheet.Columns(0).SetLongName('Time')
sheet.Columns(0).SetType(PyOrigin.COLTYPE_DESIGN_X)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, 0, -1, 0)
for i in range(1, len(df_norm[0])):
sheet.Columns(i).SetLongName('Delta F / n')
sheet.Columns(i).SetUnits('kHz/cm^2')
sheet.Columns(i).SetComments(str((i-1)*2+1))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_Y)
rng.Add('Y', sheet, 0, i, -1, i)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
# delta D
# create worksheet and plot
sheet = get_sheet(file+'_dd', dd_norm)
gl, rng = get_plot(file+'_dd')
sheet.Columns(0).SetLongName('Time')
sheet.Columns(0).SetType(PyOrigin.COLTYPE_DESIGN_X)
# graph worksheet's i col as X
rng.Add('X', sheet, 0, 0, -1, 0)
for i in range(1, len(dd_norm[0])):
sheet.Columns(i).SetLongName('Delta D')
sheet.Columns(i).SetUnits('x 10^-6')
sheet.Columns(i).SetComments(str((i-1)*2+1))
sheet.Columns(i).SetType(PyOrigin.COLTYPE_DESIGN_Y)
rng.Add('Y', sheet, 0, i, -1, i)
dp = gl.AddPlot(rng, 200)
PyOrigin.LT_execute('layer -g')
else:
pass
# save origin file
PyOrigin.Save(save_origin_filename)
else:
pass
# quit origin
# quit()