CS计算机代考程序代写 python Euler_Bernoulli_Handout

Euler_Bernoulli_Handout

Advanced Structural Analysis and Dynamics 5 – ENG5274¶
Course Work 1 – Euler–Bernoulli Beam Theory¶
February 10 2021
Andrew McBride

In [ ]:

import numpy as np
import matplotlib.pyplot as plt
import math

Overview¶
In this report, you will develop and validate a finite element code written in Python for solving Euler–Bernoulli beam theory.
The code will extend the one you developed for a linear elastic bar in 1D.

The report is to be uploaded to Moodle by 8 March 2020 (by 15:00).

Submission requirements¶
Report¶
The main report document should clearly and logically address all the tasks. Marks will be deducted for poor presentation. The report is to be submitted on-line via Moodle – hard-copies will not be marked.

You are to write the report in the Jupyter Notebook format (IPython) using Markdown for the written report.
You can use Google Colab, Jupyter Notebook or your favourite IPython file editor.

You need to submit:

the main_EB.ipynb containing the write up and code.
No other documents will be accepted.

Code¶
Your code needs to be commented and documented.
You must include the validation examples in your submission.

Primary functions¶
Primary functions to compute the element stiffness matrix \$mathbf{K}^e\$, the element force vector due to distributed loading \$mathbf{f}_Omega^e\$ and the local to global degree of freedom map.

In [1]:

def get_Ke(le, EIe):
”’Return element stiffness matrix
Parameters
———-
le : double
Length of element
EIe : double
Product of Young’s modulus and moment of inertia
”’
return

def get_fe_omega(le, fe):
Parameters
———-
le : double
Length of element
fe : double
”’
return

def get_dof_index(e):
”’Return the global dof associated with an element
Parameters
———-
e : int
Element ID
”’
return

Validation problems¶
Consider a 12 m beam with \$EI = 1e4\$ Nm. Ensure that your code is indeed producing the correct results by comparing the computed deflection and possibly rotation with the analytical solution for the following loading conditions:

An end-loaded cantilever beam with point load of \$P = -10\$ N acting at \$x = 12\$ m. The beam is fully fixed at \$x=0\$. Compare the computed tip deflection and rotation with the analytical solution.
A cantilever beam with a distributed load of \$f = -1\$ N/m acting over the length of the beam. The beam is fully fixed at \$x=0\$. Compare the computed tip deflection and rotation with the analytical solution.
An off-center-loaded simple beam with a point load of \$P = -10\$ N acting at \$x = 3\$ m. Deflections are 0 at \$x=0\$ and \$x=L\$. Ensure that the load acts at a node. You only need to compare your solution to the analytical solution for the position of, and deflection at, the point of maximum displacement.
A uniformly-loaded simple beam with a distributed load of \$f = -1\$ N/m acting over the length of the beam. Deflections are 0 at \$x=0\$ and \$x=L\$. You only need to compare the deflection along the length of the beam to the analytical solution.

Where possible, you should test your code for one element and for multiple elements.

Validation – Cantilever with point load¶

In [2]:

# properties of EB theory
dof_per_node = 2

# domain data
L = 12.

P = -10.
P_x = L
f_e = 0.
EI = 1e4

# mesh data
n_el = 1
n_np = n_el + 1
n_dof = n_np * dof_per_node
x = np.linspace(0, L, n_np)
le = L / n_el

K = np.zeros((n_dof, n_dof))
f = np.zeros((n_dof, 1))

for ee in range(n_el):
dof_index = get_dof_index(ee)
K[np.ix_(dof_index, dof_index)] += get_Ke(le, EI)
f[np.ix_(dof_index)] += get_fe_omega(le, f_e)

node_P = np.where(x == P_x)[0][0]
f[2*node_P] += P
free_dof = np.arange(2,n_dof)
K_free = K[np.ix_(free_dof, free_dof)]
f_free = f[np.ix_(free_dof)]

# solve the linear system
w_free = np.linalg.solve(K_free,f_free)
w = np.zeros((n_dof, 1))
w[2:] = w_free

# reaction force
rw = K[0,:].dot(w) – f[0]
rtheta = K[1,:].dot(w) – f[1]

# analytical solution
w_analytical = (P * L**3) / (3*EI)
theta_analytical = (P * L**2) / (2*EI)

print(‘————————————‘)
print(‘Reaction force: ‘, rw, ‘ Reaction moment: ‘, rtheta)
print(‘Computed tip deflection: ‘, w[-2], ‘ Analytical tip deflection: ‘, w_analytical)
print(‘Computed tip rotation: ‘, w[-1], ‘ Analytical tip rotation: ‘, theta_analytical)

plt.plot(x,w[0::2],’k-*’)
plt.xlabel(‘position (x)’)
plt.ylabel(‘deflection (w)’)
plt.show()

plt.plot(x,w[1::2],’k-*’)
plt.xlabel(‘position (x)’)
plt.ylabel(‘rotation (w)’)
plt.show()

—————————————————————————
NameError Traceback (most recent call last)
in
15 n_np = n_el + 1
16 n_dof = n_np * dof_per_node
—> 17 x = np.linspace(0, L, n_np)
18 le = L / n_el
19

NameError: name ‘np’ is not defined

Validation – Cantilever with distributed load¶

In [3]:

P = 0.
f_e = -1.

# mesh data
n_el = 10
n_np = n_el + 1
n_dof = n_np * dof_per_node
x = np.linspace(0, L, n_np)
le = L / n_el

K = np.zeros((n_dof, n_dof))
f = np.zeros((n_dof, 1))

for ee in range(n_el):
dof_index = get_dof_index(ee)
K[np.ix_(dof_index, dof_index)] += get_Ke(le, EI)
f[np.ix_(dof_index)] += get_fe_omega(le, f_e)

free_dof = np.arange(2,n_dof)
K_free = K[np.ix_(free_dof, free_dof)]
f_free = f[np.ix_(free_dof)]

# solve the linear system
w_free = np.linalg.solve(K_free,f_free)
w = np.zeros((n_dof, 1))
w[2:] = w_free

# reaction force
rw = K[0,:].dot(w) – f[0]
rtheta = K[1,:].dot(w) – f[1]

# analytical solution
w_analytical = (f_e * L**4) / (8*EI)
theta_analytical = (f_e * L**3) / (6*EI)

print(‘Validation: cantilever with uniformly distributed load’)
print(‘——————————————————‘)
print(‘Reaction force: ‘, rw, ‘ Reaction moment: ‘, rtheta)
print(‘Computed tip deflection: ‘, w[-2], ‘ Analytical tip deflection: ‘, w_analytical)
print(‘Computed tip rotation: ‘, w[-1], ‘ Analytical tip rotation: ‘, theta_analytical)

plt.plot(x,w[0::2],’k-*’)
plt.xlabel(‘position (x)’)
plt.ylabel(‘deflection (w)’)
plt.show()

plt.plot(x,w[1::2],’k-*’)
plt.xlabel(‘position (x)’)
plt.ylabel(‘rotation (w)’)
plt.show()

—————————————————————————
NameError Traceback (most recent call last)
in
7 n_np = n_el + 1
8 n_dof = n_np * dof_per_node
—-> 9 x = np.linspace(0, L, n_np)
10 le = L / n_el
11

NameError: name ‘np’ is not defined

In [ ]:

In [ ]:

P = 0.
P_x = 3.
f_e = -1.
EI = 1e4

Now consider the \$L = 12\$ m beam shown below. The beam is fully fixed at point A \$(x = 0)\$. A distributed load of \$f(x) = -1\$ N/m acts between points A and B. Point loads \$P_1 = -10\$ N and \$P_2 = 5\$ N act at \$x = 4\$ m and \$x = 8\$ m, respectively. Natural boundary conditions are comprised of a traction \$overline{Q} = -20\$ N and a moment \$overline{M} = 20\$ Nm both acting at point C \$(x = L)\$. The product \$EI = 1e4\$ Nm\${}^2\$.

Assumptions¶
The code you develop for this problem should assume that the number of elements is a multiple of 3. This will ensure that the point loads are applied directly at a node (why is this important?).

Outputs¶

Determine the reaction force and moment at point A (for 12 elements). Use these to confirm that your output is correct.
Plot the deflection \$w\$ over the length of the beam (for 12 elements).
Plot the rotation \$mathsf{d} w / mathsf{d} x\$ over the length of the beam (for 12 elements).
Plot the bending moment \$M\$ over the length of the beam (for 12 elements).

In [ ]:

Problem B is identical to that considered in Problem A but the distributed load is given by
egin{align}
f(x) = sin (pi x / 8) && ext{for} && 0 leq x leq 8 , .
end{align}
Furthermore, the material properties are no longer constant and
egin{align}
EI = 1e4 (13 – x), ext{ Nm}^2 , .
end{align}

For meshes of \$3,3^2,3^3,3^4\$ elements, generate plots of

deflection (at \$x=4\$ m) versus the number of degrees of freedom.
\$ sqrt{int_0^ell w^2(x) , mathsf{d} x}\$ versus the number of degrees of freedom.

Explain the method you have used to perform the numerical integration – provide a validation example that shows your method works.

Comment on the convergence of the solution.

In [ ]: