一些小细节的修改。
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47
main.py
47
main.py
@@ -7,7 +7,7 @@ import timeit
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def egm():
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h_g_avr_sag = 11.67 * 2 / 3
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h_c_avr_sag = 14.43 * 2 / 3
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h_whole = 260 # 杆塔全高
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h_whole = 40 # 杆塔全高
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voltage_n = 3 # 工作电压分成多少份来计算
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td = 20 # 雷暴日
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insulator_c_len = 6.8 # 串子绝缘长度
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@@ -36,33 +36,38 @@ def egm():
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rg_x = None
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rg_y = None
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cad = Draw()
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# 跳闸率 利用Q╱GDW 11452-2015 架空输电线路防雷导则的公式 Ng=0.023*Td^(1.3) 20天雷暴日地闪密度为1.13
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ng = func_ng(td)
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n_sf_phases = np.zeros((phase_n, voltage_n)) # 计算每一相的跳闸率
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for phase_conductor in range(phase_n):
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rs_x = gc_x[phase_conductor]
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rs_y = gc_y[phase_conductor]
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rc_x = gc_x[phase_conductor + 1]
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rc_y = gc_y[phase_conductor + 1]
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if np.any(np.array(gc_y) < 0):
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print("导线可能掉地面了,程序退出。")
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return 0
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for phase_conductor_foo in range(phase_n):
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exposed_curve_shielded = False
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rs_x = gc_x[phase_conductor_foo]
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rs_y = gc_y[phase_conductor_foo]
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rc_x = gc_x[phase_conductor_foo + 1]
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rc_y = gc_y[phase_conductor_foo + 1]
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if phase_n == 1:
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rg_type = "g"
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if phase_n > 1: # 多回路
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if phase_conductor < 2:
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if phase_conductor_foo < 2:
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rg_type = "c"
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rg_x = gc_x[phase_conductor + 2]
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rg_y = gc_y[phase_conductor + 2]
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rg_x = gc_x[phase_conductor_foo + 2]
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rg_y = gc_y[phase_conductor_foo + 2]
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else:
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rg_type = "g"
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# TODO 保护角公式可能有问题,后面改
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shield_angle = (
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math.atan(rc_x / ((rc_y - rs_y) + string_c_len)) * 180 / math.pi
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math.atan((rc_x - rs_x) / ((rs_y - rc_y) + string_c_len)) * 180 / math.pi
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) # 保护角
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print(f"保护角{shield_angle:.3f}°")
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print(f"最低相防护标识{rg_type}")
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ng = func_ng(td)
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for u_bar in range(voltage_n):
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u_ph = (
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math.sqrt(2) * 750 * math.cos(2 * math.pi / voltage_n * u_bar) / 1.732
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) # 运行相电压
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print(f"计算第{phase_conductor + 1}相,电压为{u_ph:.2f}kV")
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print(f"计算第{phase_conductor_foo + 1}相,电压为{u_ph:.2f}kV")
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# 迭代法计算最大电流
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i_max = 0
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i_min = min_i(insulator_c_len, u_ph / 1.732)
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@@ -151,17 +156,21 @@ def egm():
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)
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if distance > rc:
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print("暴露弧已经完全被屏蔽")
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exposed_curve_shielded = True
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break
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if phase_conductor == 2:
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cad.draw(i_min, u_ph, rs_x, rs_y, rc_x, rc_y, rg_x, rg_y, rg_type, 2)
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cad.draw(i_max, u_ph, rs_x, rs_y, rc_x, rc_y, rg_x, rg_y, rg_type, 6)
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cad.save()
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# if phase_conductor_foo == 2:
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cad.draw(i_min, u_ph, rs_x, rs_y, rc_x, rc_y, rg_x, rg_y, rg_type, 2)
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cad.draw(i_max, u_ph, rs_x, rs_y, rc_x, rc_y, rg_x, rg_y, rg_type, 6)
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cad.saveas(f"egm{phase_conductor_foo+1}.dxf")
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# 判断是否导线已经被完全保护
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if abs(i_max - _max_i) < 1e-5:
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print("无法找到最大电流,可能是杆塔较高。")
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print(f"最大电流设置为自然界最大电流{i_max}kA")
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print(f"最大电流为{i_max:.2f}")
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print(f"最小电流为{i_min:.2f}")
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if exposed_curve_shielded:
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print("暴露弧已经完全被屏蔽,不会跳闸。")
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continue
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curt_fineness = 0.1 # 电流积分细度
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if i_min > i_max or abs(i_min - i_max) < curt_fineness:
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print("最大电流小于最小电流,没有暴露弧。")
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@@ -204,11 +213,9 @@ def egm():
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# if abs(calculus-0.05812740052770032)<1e-5:
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# abc=123
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# pass
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n_sf = (
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2 * ng / 10 * calculus
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) # 跳闸率 利用Q╱GDW 11452-2015 架空输电线路防雷导则的公式 Ng=0.023*Td^(1.3) 20天雷暴日地闪密度为1.13
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n_sf = (2 * ng / 10 * calculus) * arc_possibility(750, insulator_c_len)
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avr_n_sf += n_sf / voltage_n
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n_sf_phases[phase_conductor][u_bar] = n_sf
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n_sf_phases[phase_conductor_foo][u_bar] = n_sf
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print(f"工作电压为{u_ph:.2f}kV时,跳闸率是{n_sf:.6}")
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print(f"跳闸率是{avr_n_sf:.6f}")
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print(f"不同相跳闸率是{np.mean(n_sf_phases,axis=1)}")
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