3Differential Equations and Stability
In later chapters we will derive models of motors, carts, inverted pendulums, etc. using first principles of physics. The model of each of these systems will turn out to be a differential equation. To later deal with these models we use this chapter to see how differential equations are solved using Laplace transforms. We will next look at the stability of these differential equation system models. For example, keeping an inverted pendulum upright is the problem of making sure the closed‐loop differential equation describing the inverted pendulum is stable.
3.1 Differential Equations
Consider the differential equation
Recall that if then It then follows that
We next take the Laplace transform of both sides of (3.1) to obtain
or
Collecting terms this becomes
or finally
The zero input response is the inverse Laplace transform ...
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