diff --git a/NumFinSeries/NumFinSeries2/Exercise sheet 2.pdf b/NumFinSeries/NumFinSeries2/Exercise sheet 2.pdf
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diff --git a/NumFinSeries/NumFinSeries2/FEM_heat.py b/NumFinSeries/NumFinSeries2/FEM_heat.py
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+++ b/NumFinSeries/NumFinSeries2/FEM_heat.py
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+import matplotlib.pyplot as plt
+import numpy as np
+import numpy.linalg as lin
+import scipy.sparse as sp
+from scipy.sparse.linalg import spsolve
+
+
+def kappa_integral(x,y):
+    # todo 3 a)
+    return 0.5 * (y**2 - x**2) + y -x
+
+
+def build_massMatrix(N):
+    # todo 3 b)
+    M = np.identity(N)
+    return M
+
+
+def build_rigidityMatrix(N):
+    # todo 3 b)
+    # Be careful with the indices!
+    # kappa_integral could be helpful here
+    
+    M = np.zeros((N,N))
+    h = 1/(N+1)
+    
+    # The case of i=j
+    for i in range(N):
+        M[i,i] = kappa_integral((h-1)*i, h*i) \
+            + kappa_integral(h*i, (h+1)*i)
+        # to be filled
+
+    # The case of i-j=1
+    for i in range(1,N):
+        M[i, i-1] = - kappa_integral(h*i, h*(i+1))# to be filled
+
+    # The case of j-i=1
+    for i in range(N-1):
+        M[i, i+1] = - kappa_integral(h*(i-1),h*i)# to be filled
+
+    return M
+
+
+def f(t,x):
+    # todo 3 c)
+    return ((x + 1) * np.pi **2 - 1) * np.exp(-t) * np.sin(np.pi * x) - np.pi * np.exp(-t) * np.cos(np.pi * x)
+    
+
+def initial_value(x):
+    # todo 3 c)
+    return np.sin(np.pi * x)
+
+
+def exact_solution_at_1(x):
+    # todo 3 c)
+    return np.exp(-1) * np.sin(np.pi * x)
+
+
+def build_F(t,N):
+    # todo 3 d)
+    h = 1/(N+1)
+    x = np.linspace(0,1,N+1)
+    return h/3 * (f(t, x - h/2) + f(t,x) + f(t, x + h/2))
+
+
+def FEM_theta(N,M,theta):
+    # todo 3 e)
+    h = 1/(N+1)
+    k = 1/(M+1)
+    u = initial_value(np.linspace(0,1,N+1))
+    M_matrix = build_massMatrix(N)
+    B = theta * M_matrix
+    C = (1 - theta) * M_matrix - k * build_rigidityMatrix(N)
+    F = build_F(0,N)
+    for m in range(M):
+        if (theta != 0):
+            u = np.linalg.solve(B, C @ u + F)
+        elif (theta == 0):
+            u = C @ u + F
+        F = build_F(m*k,N)
+    return u
+
+#### error analysis ####
+nb_samples = 5
+exponents = np.arange(2,7)
+N = np.pow(2,exponents) - 1 # fill in this line for f)-g)
+M = np.pow(2, exponents) # fill in this line for f)-g)
+theta= .3# fill in this line for f)-g)
+
+
+#### Do not change any code below! ####
+l2error = np.zeros(nb_samples) 
+k =  1 / M
+
+try:
+   for i in range(nb_samples):
+      l2error[i] = (1 / (N[i]+1)) ** (1 / 2) * lin.norm(exact_solution_at_1((1/(N[i]+1))*(np.arange(N[i])+1)) - FEM_theta(N[i], M[i],theta), ord=2)
+      if np.isnan(l2error[i])==True:
+          raise Exception("Error unbounded. Plots not shown.")
+   conv_rate = np.polyfit(np.log(k), np.log(l2error), deg=1)
+   if conv_rate[0]<0:
+       raise Exception("Error unbounded. Plots not shown.")
+   print(f"FEM method with theta={theta} converges: Convergence rate in discrete $L^2$ norm with respect to time step $k$: {conv_rate[0]}")
+   plt.figure(figsize=[10, 6])
+   plt.loglog(k, l2error, '-x', label='error')
+   plt.loglog(k, k, '--', label='$O(k)$')
+   plt.loglog(k, k**2, '--', label='$O(k^2)$')
+   plt.title('$L^2$ convergence rate', fontsize=13)
+   plt.xlabel('$k$', fontsize=13)
+   plt.ylabel('error', fontsize=13)
+   plt.legend()
+   plt.plot()
+   plt.show()
+except Exception as e:
+    print(e)
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