e30.in

三维矢量有限元-矩量法电磁场分析程序。 EMAP5 is a full-wave electromagnetic field solver that combines the method of m

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0.093500	0.010000	0.000000	
0.096000	0.010000	0.000000	
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0.101000	0.010000	0.000000	
0.103500	0.010000	0.000000	
0.106000	0.010000	0.000000	
0.108500	0.010000	0.000000	
0.111000	0.010000	0.000000	
0.113500	0.010000	0.000000	
0.116000	0.010000	0.000000	
0.118500	0.010000	0.000000	
0.121000	0.010000	0.000000	
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0.063500	0.010500	0.000000	
0.066000	0.010500	0.000000	
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0.156000	0.010500	0.000000	
0.158500	0.010500	0.000000	
0.161000	0.010500	0.000000	


# Global Edge Table
1	2	1	0	0	0	
2	3	1	1	0	0	
3	4	1	2	0	0	
4	5	1	3	0	0	
5	6	1	4	0	0	
6	7	1	5	0	0	
7	8	1	6	0	0	
8	9	1	7	0	0	
9	10	1	8	0	0	
10	11	1	9	0	0	
11	12	1	10	0	0	
12	13	1	11	0	0	
13	14	1	12	0	0	
14	15	1	13	0	0	
15	16	1	14	0	0	
16	17	1	15	0	0	
17	18	1	16	0	0	
18	19	1	17	0	0	
19	20	1	18	0	0	
20	21	1	19	0	0	
1	22	1	20	0	0	
1	23	1	21	0	0	
2	23	1	22	0	0	
3	23	1	23	0	0	
3	24	1	24	0	0	
3	25	1	25	0	0	
4	25	1	26	0	0	
5	25	1	27	0	0	
5	26	1	28	0	0	
5	27	1	29	0	0	
6	27	1	30	0	0	
7	27	1	31	0	0	
7	28	1	32	0	0	
7	29	1	33	0	0	
8	29	1	34	0	0	
9	29	1	35	0	0	
9	30	1	36	0	0	
9	31	1	37	0	0	
10	31	1	38	0	0	
11	31	1	39	0	0	
11	32	1	40	0	0	
11	33	1	41	0	0	
12	33	1	42	0	0	
13	33	1	43	0	0	
13	34	1	44	0	0	
13	35	1	45	0	0	
14	35	1	46	0	0	
15	35	1	47	0	0	
15	36	1	48	0	0	
15	37	1	49	0	0	
16	37	1	50	0	0	
17	37	1	51	0	0	
17	38	1	52	0	0	
17	39	1	53	0	0	
18	39	1	54	0	0	
19	39	1	55	0	0	
19	40	1	56	0	0	
19	41	1	57	0	0	
20	41	1	58	0	0	
21	41	1	59	0	0	
21	42	1	60	0	0	
22	23	1	61	0	0	
23	24	1	62	0	0	
24	25	1	63	0	0	
25	26	1	64	0	0	
26	27	1	65	0	0	
27	28	1	66	0	0	
28	29	1	67	0	0	
29	30	1	68	0	0	
30	31	1	69	0	0	
31	32	1	70	0	0	
32	33	1	71	0	0	
33	34	1	72	0	0	
34	35	1	73	0	0	
35	36	1	74	0	0	
36	37	1	75	0	0	
37	38	1	76	0	0	
38	39	1	77	0	0	
39	40	1	78	0	0	
40	41	1	79	0	0	
41	42	1	80	0	0	
22	43	1	81	0	0	
23	43	1	82	0	0	
23	44	1	83	0	0	
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25	45	1	86	0	0	
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51	52	1	130	0	0	
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53	54	1	132	0	0	
54	55	1	133	0	0	
55	56	1	134	0	0	
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60	61	1	139	0	0	
61	62	1	140	0	0	
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43	64	1	142	0	0	
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60	81	1	176	0	0	
61	81	1	177	0	0	
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64	65	1	183	0	0	
65	66	1	184	0	0	
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80	81	1	199	0	0