{"template_model": "01-П6-идеальные-трубки.fem", "scope": "Новые размеры, условная B(H); Λ из почти идеального поля не учитывает перестройку трубок при насыщении. H(B) цепи линейно интерполируется между опубликованными узлами; FEMM использует собственную интерполяцию той же таблицы. Расхождение включает также это различие, не только трубки и неоднородность по сечению. Применимость оценивается сравнением с независимым FEMM, а не переносом утверждения книги о 5 Тл.", "algorithms": [{"source": "Буль, П6.1–П6.14, печатные с.319–324; перенесено на собственные трубки и геометрию.", "pole_U_At": 736.9158859510569, "tail_U_At": 14.51971982749669, "target_Bcenter_T": 1.45, "method": 1, "sections": 4, "half_mmf_At": 1328.372274486674, "full_mmf_At": 2656.744548973348, "rows": [{"z0_mm": 0.501, "B_out_T": 1.8529614424560108, "U_tube_At": 580.027436632987, "B_in_T": 1.4835253077328006, "delta_U_At": 37.78791036051485, "phi_in_Wb": 0.0002982804613240258, "z1_mm": 5.37525, "lambda_H": 1.28062118280952e-07, "phi_out_Wb": 0.00037256000352031677}, {"z0_mm": 5.37525, "B_out_T": 1.979091215925971, "U_tube_At": 649.4217215042838, "B_in_T": 1.8529614424560108, "delta_U_At": 123.86285964484023, "phi_in_Wb": 0.00037256000352031677, "z1_mm": 10.2495, "lambda_H": 3.904996525850225e-08, "phi_out_Wb": 0.0003979198991831758}, {"z0_mm": 10.2495, "B_out_T": 2.076640034480916, 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