Figure 1 below shows a schematic of the mass-spring-damper model to include an applied external force, F.
Figure 1.Mass-Spring-Damper system with external force
In post #5 of this series on solving 2nd order, linear ODE's, we began by constructing a free-body diagram of a typical mass-spring-damper mechanism, to derive the equation of motion for the free oscillating system - equation (1)...
We derive the equation of motion to this system in exactly the same way as in post #5.
From equation (2), we can see that the sum of the internal forces consisting of:
...are in equilibrium with the external force.
In the this and the next few posts, we are going to look at how the system responds, that is how the mass moves, when the external force is an oscillating force. That is...
Thus the equation of motion (2) becomes...
So we have a 2nd order, linear, non-homogeneous differential equation for which we can solve using the method of undetermined coefficients.
We know from equation (3) in post #8, the solution has the form...
Let's find the particular solution to the non-homogeneous equation first.
From the table 1 in post #12 above, we choose...
...then...
...and...
Sub these into (3), we get...
Equating the coefficients on both sides, we have...
Thus from (6)...
...and substituting this result into (5)...
From post #4, we found that the natural frequency of an undamped mechanism can be expressed as...
So let's express the coefficients A and B in terms of the natural frequency on an undamped system. Why? we'll find out in the next post...
Finally, the particular solution to the non-homogeneous equation is...
Alright, in the next post, we'll look at a special case - forced oscillations on an undamped system creating resonance.
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