I Justify Assumption of Exponential Response to Free Vibration Problem

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The discussion centers on the justification for assuming an exponential response in free vibration problems involving mass, damping, and springs. Participants highlight that while Euler's formula connects complex exponentials to sine and cosine functions, the initial assumption of an exponential response is rooted in the nature of differential equations. The characteristic equation derived from Newton's second law leads to solutions that include exponential terms, particularly in cases of underdamping. The conversation also touches on the utility of the Laplace transform for simplifying the solution process in electrical engineering contexts. Ultimately, the assumption of exponential solutions is acknowledged as a foundational concept in analyzing such dynamic systems.
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Why assume exponential
Consider a free vibration problem of a mass in 1D: inertia, damping, spring, and no forcing function.

We begin by assuming an exponential response.

And then run through all the cases of under, over, critical damping, etc.

I am fully aware of Euler's formula that relates sine/cosine to complex exponential, etc.

But when an analyst first attemps a solution of such a system, there is no a priori knowedge about such issues -- just a posteriori knowledge
of what it leads to.

Can someone justify why we assume a trial exponential response to a free vibration problem?

The only answer I seem able to give is that: it works because Euler, complex, trig, etc.

(Forgive me for marking this "Advanced" I seek a more conceptual understandingFor example, could one say that the derivatives of the exponential are exponential and this serves as a basis for all possible functions?
 
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Trying2Learn said:
For example, could one say that the derivatives of the exponential are exponential and this serves as a basis for all possible functions?
You hit the nail on the head (old dutch expression).

In dealing with differential equations like ##x'' + \omega^2 x = 0## it is sensible to try exponentials. See characteristic equation in calculus books.
 
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You don't need to assume any response. Newton's second law gives you a homogenous second order differential equation, $$m\ddot{x} + b \dot{x} + kx = 0$$ You can solve the complementary equation for ##\lambda## for the three different types of damping (depending on whether the discriminant ##b^2 - 4mk## is less than, equal to, or greater than zero) and come up with the equation of motion.

If you get complex ##\lambda = a \pm bi##, the complementary solution is of the form ##x = Ae^{at}\cos{(bt + \phi)}##. This is the case with underdamping!
 
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OK, you need to know Euler's equation, a priori in your words.
Then the equation given in the previous post is solved in a number of ways. The "classical" way is to assume exponential solutions. Unexplained, a priori!

If you're working towards an electrical degree you will be saved with the use of the Laplace transform. Essentially you just look up the relevand Laplace-transformed term(s) in a nice table to get the time response. SO much easier and it includes all initial conditions FOR FREE! :smile:
 
Trying2Learn said:
(Forgive me for marking this "Advanced" I seek a more conceptual understanding
No. "A" means you have a graduate school background and want to discuss the subject at the graduate school / PhD level. I will change it to "I" for you.
 
Here is a simple but intuitive way of thinking about Euler's equation and oscillations (vibrations):


I suggest watching from the beginning (and also previous lessons).
It's a bit on the basic level, but perhaps you will gain better insights.
 
thank you all. I just logged back in, and saw there were additional comments.
Thank you.
 
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