ODE with base excitation caused by a half sine wave

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Homework Help Overview

The problem involves analyzing the displacement response of a car's suspension system subjected to periodic half sine wave road bumps. The system is characterized by its stiffness and effective mass, with the assumption of negligible damping. The Fourier series representation of the road profile is provided, which introduces complexity in the analysis of the system's response.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the application of the superposition principle to solve the differential equation governing the system's response. There are attempts to separate the problem into manageable parts, focusing on individual terms of the Fourier series. Some participants express uncertainty about the correctness of their solutions, particularly regarding the final term involving the cosine series.

Discussion Status

There is ongoing dialogue about potential sign errors in the calculations, with participants suggesting that the original poster verify their work. Some guidance has been offered regarding the formulation of the solution, but no consensus has been reached on the correctness of the final expression for the displacement response.

Contextual Notes

Participants are navigating the complexities of the Fourier series representation and its implications for the solution. There is a noted difficulty in verifying certain terms, which may be affecting the overall confidence in the proposed solutions.

Dustinsfl
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Homework Statement


The suspension system of a car traveling on a bumpy road has a stiffness of ##k = 5\times 10^6## N/m and the effective mass of the car on the suspension is ##m = 750## kg. The road bumps can be considered to be periodic half sine waves with period ##\tau##. Determine the displacement response of the car. Assume the damping of the system to be negligible. Hint: The Fourier series representation of the bumpy road, ##y(t)##, is given by
$$
y(t) = \frac{1}{\pi} + \frac{1}{2}\sin(2\pi t) - \frac{2}{\pi}
\Big(\frac{\cos(4\pi t)}{3} + \frac{\cos(8\pi t)}{15} +
\frac{\cos(12\pi t)}{35} + \cdots\Big)
$$

Homework Equations


$$
\frac{2}{\pi}
\Big(\frac{\cos(4\pi t)}{3} + \frac{\cos(8\pi t)}{15} +
\frac{\cos(12\pi t)}{35} + \cdots\Big) = \frac{2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4j\pi t)}{4j^2 - 1}
$$

The Attempt at a Solution


If I solve each piece separately and use the superposition principle, the first two terms work as solution but I can't verify that the final piece is so I am assuming something is wrong.
\begin{align*}
750\ddot{x} + 5\times 10^6x
&= \frac{1}{\pi} + \frac{1}{2}\sin(2\pi t) - \frac{2}{\pi}
\sum_{j = 1}^{\infty}\frac{\cos(4j\pi t)}{4j^2 - 1}\\
750\ddot{x} + 5\times 10^6x &= \frac{1}{\pi}\\
x_{p1}(t) &= \frac{1}{5\times 10^6\pi}\\
750\ddot{x} + 5\times 10^6x &= \frac{1}{2}\sin(2\pi t)
\end{align*}
Here we will let ##x_{p2} = A\cos(2\pi t) + B\sin(2\pi t)## Then
$$
A\cos(2\pi t)\big[5\times 10^6 - 3000\pi^2\big] +
B\sin(2\pi t)\big[5\times 10^6 - 3000\pi^2\big]
= \frac{1}{2}\sin(2\pi t)
$$
Therefore, ##A = 0## and ##B = \frac{1}{10\times 10^6 - 6000\pi^2}##.
\begin{align*}
x_{p2}(t) &= \frac{1}{10\times 10^6 - 6000\pi^2}\sin(2\pi t)\\
750\ddot{x} + 5\times 10^6x
&= \frac{-2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4j\pi t)}{4j^2 - 1}
\end{align*}
No matter how I have tried to solve this final piece, the solution doesn't seem to work out though. I end up getting ##A_j = \frac{-2}{\pi(k-16\pi^2j^2m)}## and ##B = 0##. Then
$$
\frac{-2}{\pi(k-16\pi^2j^2m)}\cos(4\pi jt) + 0\sin(4\pi j t) = \cos(4\pi j t - \phi_j)
$$
Therefore, ##\phi = \tan^{-1}(0/A) = 0## and ##R = \sqrt{A^2 + B^2} = \frac{2}{\pi(k-16\pi^2j^2m)}\cos(4\pi jt)##.
$$
x_{p3} = \frac{2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4\pi j t)}{k-16\pi^2j^2m}
$$
and
$$
x_p(t) = \frac{1}{5\times 10^6\pi} + \frac{1}{10\times 10^6 - 6000\pi^2}\sin(2\pi t) + \frac{2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4\pi j t)}{5*10^6-12000\pi^2j^2}
$$
but I am unable to verify
$$
\frac{2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4\pi j t)}{5*10^6-12000\pi^2j^2}
$$
as a solution so I don't think it is correct.
 
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I think you made a sign error, but otherwise, everything looks fine. How are you trying to verify the solution?
 
vela said:
I think you made a sign error, but otherwise, everything looks fine. How are you trying to verify the solution?

Differentiating twice x_{p3}times m + k times x_{p3} = RHS sum
 
Dustinsfl said:
$$750\ddot{x} + 5\times 10^6x = \frac{-2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4j\pi t)}{4j^2 - 1}$$ No matter how I have tried to solve this final piece, the solution doesn't seem to work out though. I end up getting ##A_j = \frac{-2}{\pi(k-16\pi^2j^2m)}## and ##B = 0##.
You don't need to do the next step of finding a phase angle. You can write down the solution immediately:
$$ x_{p3} = \sum_{j=1}^\infty [A_j \cos(4\pi jt) + B_j \sin(4\pi jt)] = \sum_{j=1}^\infty-\frac{2}{\pi(k-16\pi^2j^2m)}\cos (4\pi j t).$$
Then
$$\frac{-2}{\pi(k-16\pi^2j^2m)}\cos(4\pi jt) + 0\sin(4\pi j t) = \cos(4\pi j t - \phi_j).$$ Therefore, ##\phi = \tan^{-1}(0/A) = 0## and ##R = \sqrt{A^2 + B^2} = \frac{2}{\pi(k-16\pi^2j^2m)}\cos(4\pi jt)##.
The sign error crept in here. You should have gotten ##\phi_j = \pi## because you ended up with R = -A. In fact, you need to be a little more careful. The way you defined R, you have R = |A| because the principal square root is always positive, so depending on the sign of A, R could be +A or -A.
$$x_{p3} = \frac{2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4\pi j t)}{k-16\pi^2j^2m}$$ and
$$x_p(t) = \frac{1}{5\times 10^6\pi} + \frac{1}{10\times 10^6 - 6000\pi^2}\sin(2\pi t) + \frac{2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4\pi j t)}{5*10^6-12000\pi^2j^2}$$
but I am unable to verify
$$\frac{2}{\pi}\sum_{j = 1}^{\infty}\frac{\cos(4\pi j t)}{5*10^6-12000\pi^2j^2}$$
as a solution so I don't think it is correct.
 
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