diff --git a/src/rotating_field.py b/src/rotating_field.py
deleted file mode 100644
index bbcfebd..0000000
--- a/src/rotating_field.py
+++ /dev/null
@@ -1,55 +0,0 @@
-import numpy as np
-import matplotlib.pyplot as plt
-
-plot_fontsize = 12
-
-in_rot_vector = [0, 0, 1]  # [-]
-in_rotcenter = [0, 0, 0]  # [uT]
-in_rotmag = 10  # [uT]
-in_rotrate = 1  # [deg/s]
-in_timestep = 1  # [s]
-
-# Normalize rotation vector
-if np.linalg.norm(in_rot_vector)==0:
-    # ui_print("Error: Rotation axis cannot be singular.")
-    raise ValueError('Zero vector for rotation axis given!')
-else:
-    v = in_rot_vector / np.linalg.norm(in_rot_vector)
-# Find perpendiculat vectors
-if v[1] == 0 and v[2] == 0:
-    a = np.cross(v, [0, 1, 0])
-else:
-    a = np.cross(v, [1, 0, 0])
-b = np.cross(v, a)
-
-print(v)
-print(a)
-print(b)
-# Some vectors
-c = [1, 2, 3]
-r = in_rotmag
-
-# Get full rotation array
-cycle_time = (360/in_rotrate)/in_timestep
-
-arr_len = int(np.floor(cycle_time/in_timestep))
-th = 0  # [rad]
-x = np.zeros(arr_len)
-y = np.zeros(arr_len)
-z = np.zeros(arr_len)
-# Calculate vectors
-for i in range(arr_len):
-    th = th+in_rotrate*np.pi/180
-    x[i] = in_rotcenter[0] + in_rotmag*np.cos(th)*a[0]+r*np.sin(th)*b[0]
-    y[i] = in_rotcenter[1] + in_rotmag*np.cos(th)*a[1]+r*np.sin(th)*b[1]
-    z[i] = in_rotcenter[2] + in_rotmag*np.cos(th)*a[2]+r*np.sin(th)*b[2]
-
-ax = plt.figure().add_subplot(projection='3d')
-ax.plot(x[0], y[0], z[0], 'o', color='blue')
-ax.plot(x, y, z, label='curve in (x, y,z)')
-ax.plot(x[arr_len-1], y[arr_len-1], z[arr_len-1], '^', color='red')
-ax.set_xlabel(r'$B_x [{\mu}T]$', fontsize=plot_fontsize)
-ax.set_ylabel(r'$B_y [{\mu}T]$', fontsize=plot_fontsize)
-ax.set_zlabel(r'$B_z [{\mu}T]$', fontsize=plot_fontsize)
-plt.show()
-