/
varjena_cev_FEM_working.py
497 lines (358 loc) · 14.4 KB
/
varjena_cev_FEM_working.py
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
import numpy as np
from scipy.integrate import quad
from numpy.linalg import solve
import matplotlib
from matplotlib import pyplot as plt
np.set_printoptions(precision=5)
#Podatki: ---------------------------------------------------------------------
#Material
E_jeklo = 2.1e5 #[MPa]
nu_jeklo = 0.3
E_zvar = 2.05e5 #[MPa]
nu_zvar = 0.3
sigma_tec = 250 #[MPa] (ASTM A36 jeklo)
SF = 0.5 #[/] faktor varnosti
koef_zvara = 0.7 #[/] sigma_dop_zvar = sigma_dop * koef_zvara
#Geometrija
d_o = 1016 #[mm]
t = 9.5 #[mm]
alpha_zvar = 30 #[°] - kot žleba zvara
R_koren = 10 #[mm] - širina špranje korena zvara
#Obremenitev
p = 1 #[MPa]
# -----------------------------------------------------------------------------
#Frormat prikaza: -------------------------------------------------------------
'''
simetrija = 1: prikaz celotne cevi (simetrija y)
0: prikaz le polovice cevi
prikazi: 0 -> primerjalna napetost
1 -> sigma_xx
2 -> sigma_yy
3 -> sigma_zz
4 -> sigma_xy
5 -> epsilon_xx
6 -> epsilon_yy
7 -> epsilon_xy
(primer: prikazi = [0,1,2])
povecava = <vrednost povačave prikaza pomikov>
'''
simetrija = 1
povecava = 1
prikazi = [0]
# -----------------------------------------------------------------------------
#Uvoz (definicija) mreže: -----------------------------------------------------
mesh_import = 1 #1: uvoz mreže, 2: definiraj lastno mrežo
nodes_file = "nodes.txt"
elements_file = "elements.txt"
# -----------------------------------------------------------------------------
#Preračun vhodnih podatkov ----------------------------------------------------
r_o = d_o/2
r_i = r_o - t
dz = 1 #[mm]
sig_dop = sigma_tec * SF
sig_dop_zvar = sig_dop * koef_zvara
# Uboz mreže ------------------------------------------------------------------
def readfile(text,elements=0):
'''
text: ime datoteke s podatki o vozliščih / elementih
elements: 1, ko uvazamo datoteko z elementi (privzeto 0)
'''
lines = []
with open(text) as textfile:
for line in textfile.readlines():
line = line.translate({ord(','):None}) # odstrani ','
line = line.rstrip().split()[1:] # razdeli, odstrani 1. element
if elements:
lines.append([int(i)-1 for i in line]) #pretvori v int, odšteje 1
else:
lines.append([float(i) for i in line]) #pretvori v float
return lines
if mesh_import:
print('Uvoz mreže...\n')
nodes = readfile(nodes_file)
elements = readfile(elements_file,1)
else:
#Točke
nodes = [[0.,0.],
[0.,-r_i],
[r_i,-r_i],
[r_i,0.],
[r_i,r_i],
[0.,r_i]]
#Povezave točk - elementi:
elements = [[0,1,3],
[3,5,0],
[1,2,3],
[3,4,5]]
nodearray=np.array(nodes,dtype=float)
#Mreža:
def build_mesh(nodearray, elements):
mesh = []
for el in elements:
mesh.append([nodearray[el,:],el])
#element seznama mesh: [xy,el], "el" je seznam nodov elementa
return mesh
mesh = build_mesh(nodearray, elements)
print('Začetek analize...')
# ROBNI POGOJI --------------------------------------------------------
#Bistveni (fiksirani pomiki): -----------------------------------------
xfixed = []
for i in range(nodearray.shape[0]):
if nodearray[i][1] == 0:
zero_y = i
break
yfixed = [zero_y] #Eno vozlišče je treba fiksirati v y smeri
#Fiksirani pomiki v x smeri za vse node na simetrijski osi:
for n in range(nodearray.shape[0]):
if nodearray[n,0] == 0:
xfixed.append(n)
xvalue=np.zeros(2*nodearray.shape[0]) #zaenkrat le, če so fiksirani pomiki 0
yvalue=np.zeros(2*nodearray.shape[0])
#Iskanje vozlišč na notranjem robu cevi
def r(node):
return np.sqrt(node[0]**2+node[1]**2)
def phi(node):
return np.arctan2(node[1],node[0])
notranji = []
for n in range(nodearray.shape[0]):
if np.abs(r(nodearray[n,:])-r_i) <= r_i/10000:
notranji.append(n)
# Območje zvara (oblika trapeza - desna premica) ---------------------
k_zvar = np.tan(np.pi/2 - alpha_zvar/2/180*np.pi)
y_zvar = np.sqrt(r_i**2-(R_koren/2)**2)
T1_zvar = [R_koren/2, y_zvar]
n_zvar = T1_zvar[1]-T1_zvar[0]*k_zvar
# -------------------------------------------------------------------
class FElement(object):
''' En končni element, s koordinatami vozlišč '''
def __init__(self,mesh):
self.xy = mesh[0] #np.array 3x2, z x,y koordiantami vozlišč
self.nodes = mesh[1] #seznam vozlišč elementa
if self.is_weld(): #Če je element v območju zvara drug matrial
self.E = E_zvar
self.nu = nu_zvar
else:
self.E = E_jeklo
self.nu = nu_jeklo
self.area()
self.B()
self.D()
self.K()
self.scatter()
if self.is_inner(): #Če gre za notranji element cevi
self.f_element() #izračunaj vozliščne sile
else:
self.f_el = np.zeros(len(self.dofs)) #sicer same ničle
def area(self):
x1,y1=self.xy[0]
x2,y2=self.xy[1]
x3,y3=self.xy[2]
self.area=np.abs(1/2*(x1*(y2-y3)+x2*(y3-y1)+x3*(y1-y2)))
def B(self):
A = self.area
def beta(i):
return self.xy[i%3][1]-self.xy[(i+1)%3][1]
def gamma(i):
return self.xy[(i+1)%3][0]-self.xy[i%3][0]
BB = np.array([[beta(1),0,beta(2),0,beta(3),0],
[0,gamma(1),0,gamma(2),0,gamma(3)],
[gamma(1),beta(1),gamma(2),beta(2),gamma(3),beta(3)]],
dtype=float)
self.B = 1/(2*A)*BB
# Ravninsko deformacijsko stanje:
def D(self):
DD = np.array([[1-self.nu,self.nu,0],
[self.nu, 1-self.nu,0],
[0,0,(1-2*self.nu)/2]], dtype=float)
self.D = self.E/((1+self.nu)*(1-2*self.nu)) * DD
#Togostna matrika elementa:
def K(self):
self.K = np.dot(np.dot(np.transpose(self.B),self.D),self.B) * self.area * dz
#Vektor vozliščnih sil elementa
def f_element(self):
x1,y1 = self.notranji[0]
x2,y2 = self.notranji[1]
a = np.sqrt(np.abs(x1-x2)**2 + np.abs(y1-y2)**2)
phi_F = np.pi/2 - np.arctan(np.abs(y1-y2)/np.abs(x1-x2)) # kot lokalne voz. sile s horizontalo
F_voz = p * a/2 # velikost vozliščne sile v lokalne k. sistemu
f_el = np.zeros(len(self.dofs)) # pripravim vektor vozliščnih sil elementa
for i in self.skupni:
xsign = np.sign(np.cos(phi(self.xy[i]))) # predznak x komponente
ysign = np.sign(np.sin(phi(self.xy[0]))) # predznak y komponente
f_el[2*i] = F_voz*np.cos(phi_F) * xsign
f_el[2*i+1] = F_voz*np.sin(phi_F) * ysign
self.f_el = f_el # vektor vozliščnih sil v lokalnem k.s. elementa
#Razporeditev elementa v globalno togostno matriko:
def scatter(self):
dofs = []
for n in self.nodes:
dofs.extend((2*n,2*n+1))
self.dofs = dofs
#Ali je element na notranjem robu cevi:
def is_inner(self):
skupni = []
for i in range(len(self.nodes)):
if self.nodes[i] in notranji:
skupni.append(i)
if len(skupni)==2:
self.notranji = [self.xy[i] for i in skupni] #Dve vozlišči na notranjem robu cevi
self.skupni = skupni
return(1)
#Ali je element na območju zvara:
def is_weld(self):
self.centroid()
if self.tez[1] >= y_zvar and self.tez[0] <= (self.tez[1]-n_zvar)/k_zvar:
return 1
else: return 0
#Težišče trikotnega elementa:
def centroid(self):
self.tez = [np.sum(self.xy[:,0])/3, np.sum(self.xy[:,1])/3]
#Vsi elementi v mreži: --------------------------------------------------------
FE=[] # seznam vseh končnih elementov v mreži
for m in mesh:
FE.append(FElement(m))
#Globalna togostna matrika: ---------------------------------------------------
def build_K(FE,K_size) :
Kg = np.zeros([K_size,K_size])
for el in FE:
for i in range(len(el.dofs)):
for j in range(len(el.dofs)):
Kg[el.dofs[i],el.dofs[j]] += el.K[i,j]
return Kg
K_size = len(nodes)*2
# -----------------------------------------------------------------------------
Kg = build_K(FE,K_size)
# -----------------------------------------------------------------------------
#Vektor vozliščnih sil --------------------------------------------------------
def build_f_tlak(FE,size):
fg = np.zeros(size)
for el in FE:
for i in range(len(el.dofs)):
fg[el.dofs[i]] += el.f_el[i]
return fg
# -----------------------------------------------------------------------------
f = build_f_tlak(FE,K_size)
# -----------------------------------------------------------------------------
#Upoštevanje bistvenih robnih pogojev (preoblikovanje enačbe):
Kn = np.copy(Kg)
fn = np.copy(f)
for i in xfixed:
Kn[2*i,:]=0
Kn[:,2*i]=0
Kn[2*i,2*i]=1
fn[:]-=Kg[:,2*i]*xvalue[i]
fn[i*2]=xvalue[i]
for i in yfixed:
Kn[2*i+1,:]=0
Kn[:,2*i+1]=0
Kn[2*i+1,2*i+1]=1
fn[:]-=Kg[:,2*i+1]*yvalue[i]
fn[i*2+1]=yvalue[i]
#Rešitev sistema: -------------------------------------------------------------
U = solve(Kn,fn)
F = np.dot(Kg,U)
print('Konec analize.\n')
#Postprocesiranje: ------------------------------------------------------------
print('Postprocesiranje...\n')
#Nove koordinate vozlišč: -----------------------------------------------------
U_nodes = U.reshape(nodearray.shape)
new_nodes = nodearray + U_nodes
#Deformacije in napetosti: ----------------------------------------------------
eps = []
for element in FE:
eps.append(np.dot(element.B, U[element.dofs]))
sig = []
for i in range(len(FE)):
sig.append(np.dot(FE[i].D, eps[i]))
for i in range(len(sig)):
sig[i] = np.append(sig[i], FE[i].nu*(sig[i][0]+sig[i][1])) #sigma_zz
deformacije = np.array(eps)
napetosti = np.array(sig)
#Primerjalne napetosti (Von Mieses):
sig_VM = np.array([np.sqrt(s[0]**2+s[1]**2+s[3]**2-s[0]*s[1]-s[1]*s[3]-s[0]*s[3]+3*s[2]**2) for s in sig], dtype=float)
#Elementi zvara: --------------------------------------------------------------
zvar = []
for i in range(len(FE)):
if FE[i].is_weld():
zvar.append(i)
FE_zvar = [FE[i] for i in zvar]
sig_zvar = sig_VM[zvar]
U_zvar = [U_nodes[FE[i].nodes] for i in zvar]
#Prikaz: ----------------------------------------------------------------------
prikaz = 1
za_prikaz = [{'data': sig_VM, 'naslov': 'Primerjalna napetost'},
{'data': napetosti[:,0], 'naslov': r'$\sigma_{xx}$ [MPa]'},
{'data': napetosti[:,1], 'naslov': r'$\sigma_{yy}$ [MPa]'},
{'data': napetosti[:,3], 'naslov': r'$\sigma_{zz}$ [MPa]'},
{'data': napetosti[:,2], 'naslov': r'$\sigma_{xy}$ [MPa]'},
{'data': deformacije[:,0], 'naslov': r'$\varepsilon_{xx}$ [/]'},
{'data': deformacije[:,1], 'naslov': r'$\varepsilon_{yy}$ [/]'},
{'data': deformacije[:,2], 'naslov': r'$\varepsilon_{xy}$ [/]'}]
def plot_mesh(mesh,style,sym=0):
for m in mesh:
x = np.append(m[0][:,0], m[0][0,0])
y = np.append(m[0][:,1], m[0][0,1])
plt.plot(x,y,style)
if sym:
plt.plot(-x,y,style)
def plot_fill(value_array,title,sym=0):
x = nodearray[:,0]
y = nodearray[:,1]
triangles = np.array(elements)
if sym:
x = np.append(x,-x)
y = np.append(y,y)
triangles = np.vstack((triangles, triangles+np.amax(triangles)+1))
value_array = np.append(value_array,value_array)
plt.figure()
plt.title(title)
plt.axes().set_aspect('equal')
plt.tripcolor(x,y,triangles,value_array, edgecolors='k',cmap=plt.get_cmap('jet'))
plt.colorbar()
def plot_weld(value_array, sym=0):
x = nodearray[:,0]
y = nodearray[:,1]
triangles = np.array(elements)
xmin, xmax = (0, 1.5*R_koren/2+t*np.sin(alpha_zvar/2/180*np.pi))
ymin, ymax = (r_i-xmax/2, r_o+xmax/2)
if sym:
x = np.append(x,-x)
y = np.append(y,y)
triangles = np.vstack((triangles, triangles+np.amax(triangles)+1))
value_array = np.append(value_array,value_array)
xmin = -xmax
plt.figure()
plt.title('Primerjalna napetost v zvaru [MPa]')
plt.axes().set_aspect('equal')
axes = plt.gca()
axes.set_xlim([xmin,xmax])
axes.set_ylim([ymin,ymax])
odmik = (xmax-xmin)/50 #odmik besedila od roba
axes.text(xmin+odmik, ymin+odmik,
"Največja primerjalna napetost: {:.3f} MPa\nDopustna napetost: {:.3f} MPa".format(np.amax(sig_zvar), sig_dop_zvar))
plt.tripcolor(x,y,triangles,value_array, edgecolors='k',cmap=plt.get_cmap('jet'), vmin=0, vmax=sig_dop_zvar)
plt.colorbar()
for i in range(len(sig_zvar)):
xy_tez = FE_zvar[i].tez
axes.text(xy_tez[0], xy_tez[1], "{:.2f}".format(sig_zvar[i]), ha='center')
if sym:
axes.text(-xy_tez[0], xy_tez[1], "{:.2f}".format(sig_zvar[i]), ha='center')
def printU(element):
print(U_nodes[FE[i].nodes])
if prikaz:
print('Generiranje prikaza...')
#Elementi
plt.figure()
plt.grid()
plt.axes().set_aspect('equal')
plt.title('Deformirana oblika (faktor povečave: {:.1f})'.format(povecava))
plot_mesh(mesh, '--k', sym=simetrija)
deformed = build_mesh(nodearray + U_nodes*povecava, elements)
plot_mesh(deformed, '-b', sym=simetrija)
plot_mesh([deformed[i] for i in zvar],'-r', sym=simetrija) #elementi zvara
#Napetosti, specifične deformacije:
for dataset in [za_prikaz[i] for i in prikazi]:
plot_fill(dataset['data'], dataset['naslov'], sym=simetrija)
#Približani elementi zvara
plot_weld(sig_VM,sym=simetrija)
plt.show()