Repository navigation
Expand file tree
/
Copy pathcleaned_data.json
More file actions
1690 lines (1690 loc) · 56.9 KB
/
Copy pathcleaned_data.json
File metadata and controls
1690 lines (1690 loc) · 56.9 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
589
590
591
592
593
594
595
596
597
598
599
600
601
602
603
604
605
606
607
608
609
610
611
612
613
614
615
616
617
618
619
620
621
622
623
624
625
626
627
628
629
630
631
632
633
634
635
636
637
638
639
640
641
642
643
644
645
646
647
648
649
650
651
652
653
654
655
656
657
658
659
660
661
662
663
664
665
666
667
668
669
670
671
672
673
674
675
676
677
678
679
680
681
682
683
684
685
686
687
688
689
690
691
692
693
694
695
696
697
698
699
700
701
702
703
704
705
706
707
708
709
710
711
712
713
714
715
716
717
718
719
720
721
722
723
724
725
726
727
728
729
730
731
732
733
734
735
736
737
738
739
740
741
742
743
744
745
746
747
748
749
750
751
752
753
754
755
756
757
758
759
760
761
762
763
764
765
766
767
768
769
770
771
772
773
774
775
776
777
778
779
780
781
782
783
784
785
786
787
788
789
790
791
792
793
794
795
796
797
798
799
800
801
802
803
804
805
806
807
808
809
810
811
812
813
814
815
816
817
818
819
820
821
822
823
824
825
826
827
828
829
830
831
832
833
834
835
836
837
838
839
840
841
842
843
844
845
846
847
848
849
850
851
852
853
854
855
856
857
858
859
860
861
862
863
864
865
866
867
868
869
870
871
872
873
874
875
876
877
878
879
880
881
882
883
884
885
886
887
888
889
890
891
892
893
894
895
896
897
898
899
900
901
902
903
904
905
906
907
908
909
910
911
912
913
914
915
916
917
918
919
920
921
922
923
924
925
926
927
928
929
930
931
932
933
934
935
936
937
938
939
940
941
942
943
944
945
946
947
948
949
950
951
952
953
954
955
956
957
958
959
960
961
962
963
964
965
966
967
968
969
970
971
972
973
974
975
976
977
978
979
980
981
982
983
984
985
986
987
988
989
990
991
992
993
994
995
996
997
998
999
1000
{
"code": 200,
"message": "OK",
"data": {
"map": {
"mapName": "飞行动力学基础",
"mapDesc": "“飞行动力学基础”课程是面向我校飞行器设计与工程专业三年级本科生开设的一门核心专业课,是学生系统学习飞行动力学理论与方法的开端,课程设置为32学时,内容既涵盖理论力学、材料力学、空气动力学等基础课程的关键知识点和力学分析方法,还引入当前航天飞行器设计中的关键动力学问题,以前沿科学和工程应用为背景开展教学。\n本课程主要研究航天器力学分析中的三大基础问题,空间与时间变换部分建立了描述航天器运动的时间尺度标准和空间计量方式;牛顿第二定律以传统力学的方式建立起了以能量角度描述看待航天器作为质点运动的方法;动量矩定理增加了从动量角度描述看待航天器作为刚体姿态运动的方法。"
},
"nodeList": [
{
"nodeUid": "1843599644219805696",
"nodeName": "绪论",
"children": [
{
"nodeUid": "1843599644328857600",
"nodeName": "课程概述",
"children": [
{
"nodeUid": "1843599644425326592",
"nodeName": "课程内容与目标",
"children": []
},
{
"nodeUid": "1843599644517601280",
"nodeName": "课程资源",
"children": []
},
{
"nodeUid": "1843599644609875968",
"nodeName": "飞行器空天交会运动虚拟仿真实验",
"children": []
},
{
"nodeUid": "1844228788444073984",
"nodeName": "课后知识和能力拓展",
"children": []
}
]
},
{
"nodeUid": "1843599644702150656",
"nodeName": "课程内容与特点",
"children": [
{
"nodeUid": "1843599644827979776",
"nodeName": "课程主要内容",
"children": []
},
{
"nodeUid": "1843599644920254464",
"nodeName": "课程特点及结构安排",
"children": []
}
]
}
]
},
{
"nodeUid": "1843599645012529152",
"nodeName": "矢量与坐标变换",
"children": [
{
"nodeUid": "1843599645104803840",
"nodeName": "矢量",
"children": [
{
"nodeUid": "1843599645197078528",
"nodeName": "矢量与矢量的分量列阵",
"children": []
},
{
"nodeUid": "1843599645289353216",
"nodeName": "矢量的点乘积与叉乘积",
"children": []
}
]
},
{
"nodeUid": "1843599645381627904",
"nodeName": "坐标变换与欧拉转动定理",
"children": [
{
"nodeUid": "1843599645469708288",
"nodeName": "坐标变换",
"children": [
{
"nodeUid": "1843599645561982976",
"nodeName": "为什么要强调坐标变换?",
"children": []
},
{
"nodeUid": "1843599645654257664",
"nodeName": "坐标变换应用案例",
"children": []
}
]
},
{
"nodeUid": "1843599645746532352",
"nodeName": "基元旋转",
"children": []
},
{
"nodeUid": "1843599645834612736",
"nodeName": "一般坐标变换",
"children": [
{
"nodeUid": "1843599645939470336",
"nodeName": "若用待求角的正切函数代替正弦函数和余弦函数,那么可以抵消掉 cosθ 项,从而求解第一次和第三次转动角吗?",
"children": []
},
{
"nodeUid": "1843599646212100096",
"nodeName": "用给定顺序基元旋转实现坐标变换,会出现奇异问题。可否找出一种方法,不存在奇异?",
"children": []
}
]
},
{
"nodeUid": "1843599646124019712",
"nodeName": "欧拉转动定理",
"children": [
{
"nodeUid": "1843599646304374784",
"nodeName": "坐标变换矩阵与转轴和转角的关系",
"children": []
},
{
"nodeUid": "1843599646396649472",
"nodeName": "分析案例",
"children": []
}
]
}
]
},
{
"nodeUid": "1843599646484729856",
"nodeName": "运动系中的矢量导数",
"children": [
{
"nodeUid": "1843599646577004544",
"nodeName": "运动坐标系中矢量导数的描述方法",
"children": [
{
"nodeUid": "1843599646669279232",
"nodeName": "明确坐标系时,分量列阵可表示矢量。矢量的导数仍为矢量,如何表示为分量列阵?",
"children": []
},
{
"nodeUid": "1843599646757359616",
"nodeName": "练习",
"children": []
}
]
}
]
},
{
"nodeUid": "1843599646849634304",
"nodeName": "四元数理论",
"children": [
{
"nodeUid": "1843599646937714688",
"nodeName": "四元数的定义和性质",
"children": [
{
"nodeUid": "1843599647029989376",
"nodeName": "四元数的背景",
"children": []
},
{
"nodeUid": "1843599647122264064",
"nodeName": "四元数的定义及运算规则",
"children": []
},
{
"nodeUid": "1843599647214538752",
"nodeName": "四元数乘法",
"children": []
},
{
"nodeUid": "1843599647311007744",
"nodeName": "四元数性质",
"children": []
}
]
},
{
"nodeUid": "1843599647399088128",
"nodeName": "四元数旋转变换",
"children": []
},
{
"nodeUid": "1843599647491362816",
"nodeName": "多次四元数旋转变换的合成",
"children": []
},
{
"nodeUid": "1843599647583637504",
"nodeName": "四元数运动学方程",
"children": []
}
]
}
]
},
{
"nodeUid": "1843963305836810240",
"nodeName": "质点系的动力学方程",
"children": [
{
"nodeUid": "1857718439423119360",
"nodeName": "质点系的运动方程",
"children": [
{
"nodeUid": "1843963305945862144",
"nodeName": "惯性矩阵",
"children": [
{
"nodeUid": "1843963306038136832",
"nodeName": "背景",
"children": []
},
{
"nodeUid": "1843963306126217216",
"nodeName": "刚体运动",
"children": []
}
]
},
{
"nodeUid": "1843963306218491904",
"nodeName": "惯量椭球和惯量主轴",
"children": []
}
]
},
{
"nodeUid": "1844224266783035392",
"nodeName": "刚体的运动方程",
"children": [
{
"nodeUid": "1843963306310766592",
"nodeName": "刚体的动量矩和动能",
"children": []
},
{
"nodeUid": "1843963306403041280",
"nodeName": "刚体的动力学方程",
"children": []
},
{
"nodeUid": "1843963306491121664",
"nodeName": "自由刚体的运动特性",
"children": [
{
"nodeUid": "1843963306591784960",
"nodeName": "结论",
"children": []
}
]
},
{
"nodeUid": "1843963306679865344",
"nodeName": "一般刚体的自由转动",
"children": [
{
"nodeUid": "1843963306767945728",
"nodeName": "结论",
"children": []
}
]
},
{
"nodeUid": "1843963306860220416",
"nodeName": "本体极迹的分布规律",
"children": []
}
]
},
{
"nodeUid": "1843963306948300800",
"nodeName": "质点相对运动的动力学方程",
"children": []
}
]
},
{
"nodeUid": "1843963307036381184",
"nodeName": "分析力学基础",
"children": [
{
"nodeUid": "1843963307128655872",
"nodeName": "分析力学综述",
"children": [
{
"nodeUid": "1843963307212541952",
"nodeName": "从矢量力学到分析力学",
"children": [
{
"nodeUid": "1843963307304816640",
"nodeName": "概述",
"children": []
},
{
"nodeUid": "1843963307392897024",
"nodeName": "矢量力学与分析力学对比",
"children": []
}
]
},
{
"nodeUid": "1843963307480977408",
"nodeName": "分析力学的发展",
"children": [
{
"nodeUid": "1843963307569057792",
"nodeName": "分析力学的起源",
"children": []
},
{
"nodeUid": "1843963307657138176",
"nodeName": "近代分析力学",
"children": []
},
{
"nodeUid": "1843963307745218560",
"nodeName": "中国分析力学",
"children": []
}
]
}
]
},
{
"nodeUid": "1843963307833298944",
"nodeName": "动力学方程",
"children": [
{
"nodeUid": "1843963307921379328",
"nodeName": "动力学普遍方程",
"children": [
{
"nodeUid": "1843963308013654016",
"nodeName": "基本概念",
"children": []
},
{
"nodeUid": "1843963308101734400",
"nodeName": "动力学普遍方程表达式",
"children": []
}
]
},
{
"nodeUid": "1843963308189814784",
"nodeName": "拉格朗日方程",
"children": []
},
{
"nodeUid": "1843963308277895168",
"nodeName": "罗斯方程",
"children": [
{
"nodeUid": "1843963308365975552",
"nodeName": "小结",
"children": []
}
]
}
]
},
{
"nodeUid": "1843963308454055936",
"nodeName": "拟拉格朗日方程及其求解",
"children": [
{
"nodeUid": "1843963308550524928",
"nodeName": "准坐标与准速度",
"children": []
},
{
"nodeUid": "1843963308659576832",
"nodeName": "拟拉格朗日方程",
"children": []
},
{
"nodeUid": "1843963308747657216",
"nodeName": "拟拉格朗日方程求解",
"children": [
{
"nodeUid": "1843963308860903424",
"nodeName": "实例",
"children": []
}
]
}
]
},
{
"nodeUid": "1843963308948983808",
"nodeName": "哈密顿正则方程与正则变换",
"children": [
{
"nodeUid": "1843963309037064192",
"nodeName": "哈密顿正则方程",
"children": []
},
{
"nodeUid": "1843963309129338880",
"nodeName": "哈密顿正则方程建立",
"children": [
{
"nodeUid": "1843963309225807872",
"nodeName": "案例",
"children": []
}
]
},
{
"nodeUid": "1843963309318082560",
"nodeName": "正则变换",
"children": []
}
]
},
{
"nodeUid": "1843963309406162944",
"nodeName": "凯恩方程及其求解",
"children": [
{
"nodeUid": "1843963309498437632",
"nodeName": "凯恩方程",
"children": [
{
"nodeUid": "1843963309586518016",
"nodeName": "理论力学相关内容回顾",
"children": []
},
{
"nodeUid": "1843963309674598400",
"nodeName": "分析",
"children": []
},
{
"nodeUid": "1843963309762678784",
"nodeName": "虚功率原理",
"children": []
},
{
"nodeUid": "1843963309859147776",
"nodeName": "广义速度、偏速度、偏角速度",
"children": []
}
]
},
{
"nodeUid": "1843963309947228160",
"nodeName": "广义主动力和广义惯性力",
"children": [
{
"nodeUid": "1843963310039502848",
"nodeName": "广义主动力",
"children": []
},
{
"nodeUid": "1843963310127583232",
"nodeName": "广义惯性力",
"children": []
}
]
},
{
"nodeUid": "1843963310219857920",
"nodeName": "凯恩方程求解",
"children": [
{
"nodeUid": "1843963310307938304",
"nodeName": "实例",
"children": []
},
{
"nodeUid": "1843963310396018688",
"nodeName": "总结",
"children": []
}
]
}
]
}
]
},
{
"nodeUid": "1843963310479904768",
"nodeName": "空间运动几何与时间",
"children": [
{
"nodeUid": "1843963310576373760",
"nodeName": "地球运动与时间系统",
"children": [
{
"nodeUid": "1843963310677037056",
"nodeName": "时空观",
"children": []
},
{
"nodeUid": "1843963310765117440",
"nodeName": "物理时空观",
"children": []
},
{
"nodeUid": "1843963310853197824",
"nodeName": "传统时空观",
"children": []
},
{
"nodeUid": "1843963310970638336",
"nodeName": "地球的运动",
"children": []
},
{
"nodeUid": "1843963311058718720",
"nodeName": "时间系统",
"children": []
}
]
},
{
"nodeUid": "1843963311142604800",
"nodeName": "坐标系与地球模型",
"children": [
{
"nodeUid": "1843963311230685184",
"nodeName": "相关坐标系",
"children": []
},
{
"nodeUid": "1843963311318765568",
"nodeName": "地球模型",
"children": []
},
{
"nodeUid": "1843963311411040256",
"nodeName": "引力势",
"children": []
},
{
"nodeUid": "1843963311494926336",
"nodeName": "引力加速度",
"children": []
},
{
"nodeUid": "1843963311595589632",
"nodeName": "其它影响因素",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814797242175488",
"nodeName": "有翼导弹的运动方程",
"children": [
{
"nodeUid": "1854814797359616000",
"nodeName": "导弹概述",
"children": [
{
"nodeUid": "1854814797439307776",
"nodeName": "导弹与有翼导弹",
"children": [
{
"nodeUid": "1854814797518999552",
"nodeName": "导弹简介",
"children": []
},
{
"nodeUid": "1854814797598691328",
"nodeName": "导弹的运动",
"children": []
},
{
"nodeUid": "1854814797678383104",
"nodeName": "中国空军历史上最远距离战略运输任务",
"children": []
},
{
"nodeUid": "1854814797758074880",
"nodeName": "有翼导弹简介",
"children": []
}
]
},
{
"nodeUid": "1854814797837766656",
"nodeName": "有翼导弹举例",
"children": []
},
{
"nodeUid": "1854814797938429952",
"nodeName": "科创项目举例",
"children": [
{
"nodeUid": "1854814798018121728",
"nodeName": "北航冯如杯科技竞赛",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814798097813504",
"nodeName": "坐标系和运动变量",
"children": [
{
"nodeUid": "1854814798177505280",
"nodeName": "坐标系和运动变量的定义",
"children": [
{
"nodeUid": "1854814798341083136",
"nodeName": "地面坐标系",
"children": []
},
{
"nodeUid": "1854814798420774912",
"nodeName": "本体坐标系",
"children": []
},
{
"nodeUid": "1854814798500466688",
"nodeName": "气流速度坐标系",
"children": []
},
{
"nodeUid": "1854814798584352768",
"nodeName": "航迹速度坐标系",
"children": []
},
{
"nodeUid": "1854814798668238848",
"nodeName": "弹道坐标系",
"children": []
}
]
},
{
"nodeUid": "1854814798752124928",
"nodeName": "各坐标系之间的综合关系",
"children": [
{
"nodeUid": "1854814798836011008",
"nodeName": "从地面坐标系到本体坐标系的转换",
"children": []
},
{
"nodeUid": "1854814798915702784",
"nodeName": "从气流速度坐标系到本体坐标系的转换",
"children": []
},
{
"nodeUid": "1854814798999588864",
"nodeName": "从地面坐标系到弹道坐标系的转换",
"children": []
},
{
"nodeUid": "1854814799087669248",
"nodeName": "从弹道坐标系到航迹速度坐标系的转换",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814799167361024",
"nodeName": "作用力和力矩",
"children": [
{
"nodeUid": "1854814799247052800",
"nodeName": "作用在导弹上的力和力矩",
"children": [
{
"nodeUid": "1854814799326744576",
"nodeName": "重力",
"children": []
},
{
"nodeUid": "1854814799419019264",
"nodeName": "推力",
"children": []
},
{
"nodeUid": "1854814799502905344",
"nodeName": "空气动力",
"children": []
},
{
"nodeUid": "1854814799595180032",
"nodeName": "重心与质心的关系",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814799674871808",
"nodeName": "导弹运动动力学方程",
"children": [
{
"nodeUid": "1854814799758757888",
"nodeName": "导弹质心运动的动力学方程",
"children": [
{
"nodeUid": "1854814799842643968",
"nodeName": "动力学方程的一般投影形式",
"children": []
},
{
"nodeUid": "1854814799926530048",
"nodeName": "在地面坐标系中的运动方程",
"children": []
},
{
"nodeUid": "1854814800006221824",
"nodeName": "在本体坐标系中的运动方程",
"children": []
},
{
"nodeUid": "1854814800085913600",
"nodeName": "在航迹(弹道)坐标系中的运动方程",
"children": []
},
{
"nodeUid": "1854814800169799680",
"nodeName": "例题",
"children": []
}
]
},
{
"nodeUid": "1854814800257880064",
"nodeName": "导弹绕质心转动的动力学方程",
"children": [
{
"nodeUid": "1854814800341766144",
"nodeName": "惯性积",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814800421457920",
"nodeName": "有翼导弹的运动模型",
"children": [
{
"nodeUid": "1860990891502735360",
"nodeName": "导弹质心运动的运动学方程",
"children": []
},
{
"nodeUid": "1860990990777716736",
"nodeName": "导弹绕质心转动的运动学方程",
"children": []
},
{
"nodeUid": "1854814800501149696",
"nodeName": "导弹质量方程",
"children": [
{
"nodeUid": "1854814800580841472",
"nodeName": "变质量质系",
"children": []
}
]
},
{
"nodeUid": "1854814800668921856",
"nodeName": "导弹其它方程",
"children": []
},
{
"nodeUid": "1854814800748613632",
"nodeName": "导弹质心运动动力学方程的分析、求解流程",
"children": [
{
"nodeUid": "1854814800832499712",
"nodeName": "有关有翼导弹运动方程组的说明",
"children": []
}
]
}
]
}
]
},
{
"nodeUid": "1854814800916385792",
"nodeName": "滚转导弹的运动方程",
"children": [
{
"nodeUid": "1854814800996077568",
"nodeName": "滚转导弹简介",
"children": [
{
"nodeUid": "1854814801151266816",
"nodeName": "滚转导弹介绍",
"children": [
{
"nodeUid": "1854814801243541504",
"nodeName": "滚转导弹的分类",
"children": []
},
{
"nodeUid": "1854814801327427584",
"nodeName": "小型滚转导弹的特点",
"children": []
},
{
"nodeUid": "1854814801411313664",
"nodeName": "滚转弹道导弹的特点",
"children": []
},
{
"nodeUid": "1854814801486811136",
"nodeName": "两种滚转导弹异同点",
"children": []
},
{
"nodeUid": "1854814801570697216",
"nodeName": "滚转导弹与有翼导弹的相同点",
"children": []
},
{
"nodeUid": "1854814801650388992",
"nodeName": "滚转导弹与有翼导弹的不同点",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814801730080768",
"nodeName": "滚转导弹的坐标系",
"children": [
{
"nodeUid": "1854814801805578240",
"nodeName": "滚转导弹坐标系定义",
"children": [
{
"nodeUid": "1854814801889464320",
"nodeName": "准弹体坐标系",
"children": []
},
{
"nodeUid": "1854814801981739008",
"nodeName": "准气流速度坐标系",
"children": []
},
{
"nodeUid": "1854814802074013696",
"nodeName": "准航迹速度坐标系",
"children": []
}
]
},
{
"nodeUid": "1854814802153705472",
"nodeName": "滚转导弹坐标系之间关系",
"children": [
{
"nodeUid": "1854814802229202944",
"nodeName": "地面坐标系与准弹体坐标系",
"children": []
},
{
"nodeUid": "1854814802308894720",
"nodeName": "准弹体坐标系与准气流速度坐标系",
"children": []
},
{
"nodeUid": "1854814802388586496",
"nodeName": "弹道坐标系与准航迹速度坐标系",
"children": []
},
{
"nodeUid": "1854814802468278272",
"nodeName": "弹体坐标系与准弹体坐标系",
"children": []
}
]
},
{
"nodeUid": "1854814802543775744",
"nodeName": "滚转导弹的运动参数",
"children": []
}
]
},
{
"nodeUid": "1854814802698964992",
"nodeName": "滚转导弹的作用力和力矩",
"children": [
{
"nodeUid": "1854814802778656768",
"nodeName": "滚转导弹与有翼导弹相同的力",
"children": [
{
"nodeUid": "1854814802854154240",
"nodeName": "重力",
"children": []
},
{
"nodeUid": "1854814802933846016",
"nodeName": "推力",
"children": []
},
{
"nodeUid": "1854814803013537792",
"nodeName": "操纵力",
"children": []
},
{
"nodeUid": "1854814803093229568",
"nodeName": "空气动力",
"children": []
}
]
},
{
"nodeUid": "1854814803172921344",
"nodeName": "马格努斯力定义与特性",
"children": [
{
"nodeUid": "1854814803248418816",
"nodeName": "“香蕉球”的原因",
"children": []
},
{
"nodeUid": "1854814803328110592",
"nodeName": "马格努斯力成因",
"children": []
},
{
"nodeUid": "1854814803407802368",
"nodeName": "马格努斯效应",
"children": []
},
{
"nodeUid": "1854814803483299840",
"nodeName": "马格努斯力矩",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814803558797312",
"nodeName": "滚转导弹的运动方程及求解流程",
"children": [
{
"nodeUid": "1854814803638489088",
"nodeName": "滚转导弹的运动方程",
"children": [
{
"nodeUid": "1854814803726569472",
"nodeName": "质心运动动力学方程",
"children": []
},
{
"nodeUid": "1854814803806261248",
"nodeName": "绕质心转动动力学方程",
"children": []
},
{
"nodeUid": "1854814803881758720",
"nodeName": "运动学方程",
"children": []
}
]
},
{
"nodeUid": "1854814803961450496",
"nodeName": "滚转导弹运动方程的求解流程",
"children": []
}
]
}
]
},
{
"nodeUid": "1854814804036947968",
"nodeName": "运载火箭(弹道导弹)的运动方程",