Solving a differential equation: f = ma, f = -kx -bv

DaveMan
Messages
9
Reaction score
0
so, f = ma, and f = -kx -bv.
rearrange to the form of a differential equation.
i am stuck when the next line simply states the general solution.
i have done this for first differential only, not second derivatives.
please help!
 
Physics news on Phys.org
For the homogeneous solution to ma = -kx -bv, it is standard practice to find the characteristic equation:

First, rewrite into a standard form:

\ddot{x} + \frac{b}{m}\dot{x} + \frac{k}{m}x

Set
\frac{k}{m} = \omega_n^2

\frac{b}{m} = 2\zeta\omega_n

(the reason why should be clear by the end of the problem; natural frequency and damping ration are useful, meaningful quantities in the study of oscillations)

characteristic equation:

s^2 + 2\zeta\omega_n s + \omega_n^2 = 0

find the roots of the characteristic equation (it's just a quadratic in s), s 1,2 , so that the solution to the differential equation is written:

x(t) = C_1 e^{s_1 t} + C_2 e^{s_2 t}

using the Euler identity and some algebra, you end up with the solution:

x(t) = A e^{-\zeta\omega_n t}\cos\left(\omega_d t + \phi \right)

where the damped frequency \omega_d = \omega_n \sqrt{1-\zeta^2} and the constants A and φ (magnitude and phase) are determined by the initial conditions. (You can solve it with a sine or cosine, you'll just end up with a different phase.) That's just the basics off the top of my head, but I hope that helps.
 
I don't understand how you get the charateristic equation.
 
That's usually one of the first things you learn in an introductory differential equation course.

The linear homogeneous differential equation a y"+ by'+ cy= 0 has
"characteristic equation" ar2+ br+ c= 0.


More generally, you replace the nth derivative with rn.
 
There is the following linear Volterra equation of the second kind $$ y(x)+\int_{0}^{x} K(x-s) y(s)\,{\rm d}s = 1 $$ with kernel $$ K(x-s) = 1 - 4 \sum_{n=1}^{\infty} \dfrac{1}{\lambda_n^2} e^{-\beta \lambda_n^2 (x-s)} $$ where $y(0)=1$, $\beta>0$ and $\lambda_n$ is the $n$-th positive root of the equation $J_0(x)=0$ (here $n$ is a natural number that numbers these positive roots in the order of increasing their values), $J_0(x)$ is the Bessel function of the first kind of zero order. I...

Similar threads

Back
Top