| 123456789101112131415161718192021222324252627282930313233343536373839404142434445464748495051525354555657585960616263646566676869707172737475767778798081828384858687888990919293949596979899100101102103104105106107108109110111112113114115116117118119120121122123124125126127128129130131132133134135136137138139140141142143144145146147148149150151152153154155156157158159160161162163164165166167168169170171172173174175176177178179180181182183184185186187188189190191192193194195196197198199200201202203204205206207208209210211212213214215216217218219220221222223224225226227228229230231232233234235236237238239240241 |
- # -*- coding: utf-8 -*-
- """
- MARS SSSR 轴向磁拉力 — 正式计算
- =================================
- 第5轮探测确认: AFM 力数据在 3D lumped 力图, 命名沿用径向机惯例, 其 "Fr"
- (法向力) 在 AFM 2.5D 展开模型中即轴向力:
- Fr_Rotor_OL_Lumped / Fr_Rotor_OC_Lumped (转子, 负载/空载)
- Fr_Stator_OL_Lumped / Fr_Stator_OC_Lumped (定子, 反作用)
- 节点: 转子 10 (36°步, 首尾重复共11点), 定子 12 (30°步, 共13点); 单位 N。
- 两个径向切片 (sec1 r=28.25mm, sec2 r=34.75mm) 分别读, 节点求和+切片求和
- 得净轴向力; 按时间步扫描得波形。
- 校核: (a) 定子合力 ≈ -转子合力; (b) Σ(Ft×r) ≈ 电磁转矩图;
- (c) 解析 F ≈ A/(2μ0)·mean(B²)。
- 用法: python axial_force_final.py [--quit]
- """
- import json
- import math
- import os
- import sys
- import time
- BASE = os.path.dirname(os.path.abspath(__file__))
- MOT_SRC = os.path.join(BASE, "MARS-12S10P_SSSR_D76-C150_V5.0-0819.mot")
- OUT_DIR = os.path.join(BASE, "output_motorcad")
- MU0 = 4e-7 * math.pi
- SEC_RADII_MM = [28.25, 34.75] # AFM_SectionCentreRadius_Array
- MAX_TSTEPS = 64
- MAX_NODES = 40
- def stats(ys):
- if not ys:
- return None
- return {"mean": sum(ys) / len(ys), "min": min(ys), "max": max(ys),
- "pk2pk": max(ys) - min(ys), "n": len(ys)}
- def read_nodes(mc, graph, sec, tstep):
- """读某时间步的全部节点 (x=角度, y=力N); 首尾重复点保留由调用方处理。"""
- xs, ys = [], []
- for i in range(MAX_NODES):
- try:
- x, y = mc.get_magnetic_3d_graph_point(graph, sec, i, tstep)
- except Exception:
- break
- xs.append(x)
- ys.append(y)
- return xs, ys
- def net_force_series(mc, graph):
- """净力时间序列: 对两切片、去重节点求和; 返回 (series, meta)。"""
- series = []
- meta = {"sections": {}}
- for tstep in range(MAX_TSTEPS):
- total = 0.0
- got = False
- for sec in (1, 2):
- xs, ys = read_nodes(mc, graph, sec, tstep)
- if not ys:
- continue
- got = True
- # 首尾重复 (0°与360°同一节点) 则去掉末点
- n_unique = len(ys) - 1 if (len(xs) > 1 and
- abs(xs[-1] - xs[0] - 360.0) < 1e-6) \
- else len(ys)
- total += sum(ys[:n_unique])
- if tstep == 0:
- meta["sections"][sec] = {"n_points": len(ys),
- "n_unique": n_unique, "x": xs}
- if not got:
- break
- series.append(total)
- return series, meta
- def torque_from_ft(mc, graph):
- """t=0 时刻 Σ(Ft×r) 粗校核 (Nm)。"""
- tq = 0.0
- for sec, r_mm in zip((1, 2), SEC_RADII_MM):
- xs, ys = read_nodes(mc, graph, sec, 0)
- if not ys:
- return None
- n_unique = len(ys) - 1 if (len(xs) > 1 and
- abs(xs[-1] - xs[0] - 360.0) < 1e-6) \
- else len(ys)
- tq += sum(ys[:n_unique]) * (r_mm * 1e-3)
- return tq
- def read_2d(mc, graph, maxpts=64):
- xs, ys = [], []
- for i in range(maxpts):
- try:
- x, y = mc.get_magnetic_graph_point(graph, i)
- except Exception:
- break
- xs.append(x)
- ys.append(y)
- return xs, ys
- def main(argv):
- quit_after = "--quit" in argv
- os.makedirs(OUT_DIR, exist_ok=True)
- ts = time.strftime("%m%d_%H%M%S")
- from ansys.motorcad.core import MotorCAD, set_motorcad_exe
- # Motor-CAD 2026R1 新装机器可能未注册 MOTORCAD_ACTIVEX (pymotorcad 0.8.x
- # 仍依赖它); 此时显式定位 exe, 可用环境变量 MOTORCAD_EXE 覆盖路径。
- if not os.environ.get("MOTORCAD_ACTIVEX"):
- exe = os.environ.get(
- "MOTORCAD_EXE",
- r"D:\Program Files\ANSYS Inc\v261\motorcad\MotorCAD.exe")
- if os.path.isfile(exe):
- set_motorcad_exe(exe)
- print("启动 Motor-CAD (前台) ...")
- mc = MotorCAD()
- # /SCRIPTING 模式在部分机器上窗口创建但不显示 (任务栏有图标点不开),
- # 强制可见; 已可见时无副作用 (2026-08-26 同事复现机实测该问题)
- try:
- mc.set_visible(True)
- except Exception as e:
- print(" [提示] set_visible 失败 (不影响计算): %s" % e)
- results = {"when": ts, "source_mot": os.path.basename(MOT_SRC),
- "convention_note": ("AFM 2.5D 展开模型中 Fr(法向)=轴向力; "
- "OL=负载(RMS 21A), OC=空载开路")}
- try:
- mc.load_from_file(MOT_SRC)
- out_mot = os.path.join(OUT_DIR, "MARS_SSSR_axialF_%s.mot" % ts)
- mc.save_to_file(out_mot)
- results["work_mot"] = out_mot
- for key, names in [("RMSCurrent_A", ["RMSCurrent"]),
- ("ShaftSpeed_rpm", ["ShaftSpeed"]),
- ("Airgap_mm", ["Airgap"]),
- ("Stator_Lam_Dia_mm", ["Stator_Lam_Dia"]),
- ("Stator_Bore_mm", ["Stator_Bore"])]:
- try:
- results[key] = mc.get_variable(names[0])
- except Exception:
- results[key] = None
- for var in ["ElectromagneticForcesCalc_Load",
- "ElectromagneticForcesCalc_OC"]:
- mc.set_variable(var, True)
- print("求解 (负载点 RMS %sA, OC+OL 力同算) ..." % results["RMSCurrent_A"])
- t0 = time.time()
- mc.do_magnetic_calculation()
- results["solve_seconds"] = time.time() - t0
- print(" 耗时 %.1f s" % results["solve_seconds"])
- # ---- 净轴向力: 转子/定子 x OL/OC ----
- forces = {}
- for graph in ["Fr_Rotor_OL_Lumped", "Fr_Stator_OL_Lumped",
- "Fr_Rotor_OC_Lumped", "Fr_Stator_OC_Lumped"]:
- series, meta = net_force_series(mc, graph)
- if series:
- forces[graph] = {"series_N": series, "stats": stats(series),
- "meta": meta}
- print(" %s: %s" % (graph, stats(series)))
- else:
- forces[graph] = None
- print(" [如实] %s 无数据" % graph)
- results["axial_forces"] = forces
- # ---- 校核 a: 定转子合力反号 ----
- checks = {}
- for case in ("OL", "OC"):
- fr = forces.get("Fr_Rotor_%s_Lumped" % case)
- fs = forces.get("Fr_Stator_%s_Lumped" % case)
- if fr and fs:
- mr, ms = fr["stats"]["mean"], fs["stats"]["mean"]
- checks["action_reaction_%s" % case] = {
- "rotor_mean_N": mr, "stator_mean_N": ms,
- "imbalance_pct": abs(mr + ms) / max(abs(mr), 1e-9) * 100}
- # ---- 校核 b: Σ(Ft×r) vs 转矩 ----
- tq_ft = torque_from_ft(mc, "Ft_Rotor_OL_Lumped")
- _, tq_graph = None, None
- txs, tys = read_2d(mc, 17) # id17 = 总转矩 (第4轮已辨认)
- tq_graph = stats(tys)["mean"] if tys else None
- checks["torque_crosscheck"] = {"sum_Ft_x_r_Nm_t0": tq_ft,
- "torque_graph_mean_Nm": tq_graph}
- # ---- 校核 c: 解析 F ≈ A/(2μ0)·mean(B²), B 取气隙磁密图 ----
- bxs, bys = read_2d(mc, "FluxDensityAirgap")
- if bys:
- b2 = sum(b * b for b in bys) / len(bys)
- d_out = float(results["Stator_Lam_Dia_mm"]) * 1e-3
- d_in = float(results["Stator_Bore_mm"]) * 1e-3
- area = math.pi / 4.0 * (d_out ** 2 - d_in ** 2)
- checks["analytic"] = {"mean_B2_T2": b2, "area_m2": area,
- "F_est_N": area / (2 * MU0) * b2}
- results["checks"] = checks
- print("校核: %s" % json.dumps(checks, ensure_ascii=False, indent=1))
- # ---- CSV 波形 ----
- csv_path = os.path.join(OUT_DIR, "axial_force_%s.csv" % ts)
- with open(csv_path, "w", encoding="utf-8") as f:
- f.write("tstep,Fr_Rotor_OL_N,Fr_Stator_OL_N,"
- "Fr_Rotor_OC_N,Fr_Stator_OC_N\n")
- nmax = max(len(v["series_N"]) if v else 0
- for v in forces.values())
- for i in range(nmax):
- row = [str(i)]
- for g in ["Fr_Rotor_OL_Lumped", "Fr_Stator_OL_Lumped",
- "Fr_Rotor_OC_Lumped", "Fr_Stator_OC_Lumped"]:
- v = forces.get(g)
- row.append("%.4f" % v["series_N"][i]
- if v and i < len(v["series_N"]) else "")
- f.write(",".join(row) + "\n")
- results["csv"] = csv_path
- res_path = os.path.join(OUT_DIR, "axialforce_final_%s.json" % ts)
- with open(res_path, "w", encoding="utf-8") as f:
- json.dump(results, f, ensure_ascii=False, indent=2)
- print("RESULTS: %s" % res_path)
- print("CSV: %s" % csv_path)
- # ---- 结论摘要 ----
- for case, label in (("OL", "负载(RMS 21A)"), ("OC", "空载")):
- v = forces.get("Fr_Rotor_%s_Lumped" % case)
- if v:
- s = v["stats"]
- print("[结论] %s 转子净轴向力: 均值 %.1f N, 纹波峰峰 %.2f N"
- % (label, s["mean"], s["pk2pk"]))
- return 0
- finally:
- if quit_after:
- try:
- mc.quit()
- except Exception:
- pass
- else:
- print("[提示] Motor-CAD 保持前台打开供检查。")
- if __name__ == "__main__":
- sys.exit(main(sys.argv[1:]))
|