diff --git a/examples/ReproducableCode/temp.py b/examples/ReproducableCode/temp.py
deleted file mode 100644
index f7b6ac054693706b377ce0f95cd2a7929282fa6a..0000000000000000000000000000000000000000
--- a/examples/ReproducableCode/temp.py
+++ /dev/null
@@ -1,66 +0,0 @@
-import sys
-import os
-
-src_path = os.path.join(os.path.dirname(os.path.abspath(__file__)), '../..', 'src')
-sys.path.insert(0, src_path)
-
-from Eq04 import solve_System_4eq
-
-del sys.path[0]
-
-import matplotlib.pyplot as plt
-import numpy as np
-
-
-phi_left = 8.0
-phi_right = 0.0
-p_right = 0.0
-y_A_R = 1/3
-y_C_R = 1/3
-z_A = -1.0
-z_C = 1.0
-K = 'incompressible'
-Lambda2 = 8.553e-6
-a2 = 7.5412e-4
-
-
-
-number_cells = 1024
-refinement_style = 'log'
-rtol = 1e-8
-
-
-
-y_A, y_C, phi, p, x = solve_System_4eq(phi_left, phi_right, p_right, z_A, z_C, y_A_R, y_C_R, K, Lambda2, a2, number_cells, relax_param=0.05, x0=0, x1=1,    refinement_style='hard_log', return_type='Vector', max_iter=1_000, rtol=rtol)
-
-
-
-plt.figure()
-plt.plot(x, phi)
-plt.xlabel('x [-]')
-plt.ylabel('$\\varphi$  [-]')
-plt.xlim(0,0.05)
-plt.grid()
-plt.savefig('../../docs/source/Figures/TernaryPotential.svg')
-plt.show()
-
-plt.figure()
-plt.plot(x, p)
-plt.xlabel('x [-]')
-plt.ylabel('$p$ [-]')
-plt.xlim(0,0.05)
-plt.grid()
-plt.savefig('../../docs/source/Figures/TernaryPressure.svg')
-plt.show()
-
-plt.figure()
-plt.plot(x, y_A, label='$y_A$')
-plt.plot(x, y_C, label='$y_C$')
-plt.plot(x, 1 - y_A - y_C, label='$y_S$')
-plt.xlabel('x [-]')
-plt.ylabel('$y_\\alpha$ [-]')
-plt.xlim(0,0.05)
-plt.grid()
-plt.legend()
-plt.savefig('../../docs/source/Figures/TernaryConcentrations.svg')
-plt.show()
\ No newline at end of file