In the design and analysis of control systems, we model the control process through various mathematical representations. One of such representations is the linear time-invariant systems (LTI) - a dynamic system description by linear, constant-coefficient, differential equations.
As we've seen in lecture, we will be converting a mass-spring damper system into a LTI differential equation. For supplemental instruction, see the pdf at this link.
In the mechanical system diagram below, m is the mass, k is the spring constant, b is the friction constant, u(t) is the external applied force, and y(t) is the resulting displacement.
Similar to the derivation in lecture, we can translate this system into a system of equations with respect to time. This is called the "time-variable differential equation" used to describe the mechanical system. We've derived the equation of the system (from Newton's second law as F=ma) as follows:
Sketch and briefly describe some graphs like the one about showing the response for a PID controller with:
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