lazyaditya said:
Why do you have used (s + αωn) i mean how do you have "αωn" as a root of the characteristic equation ?
Good question.
α is a new, dimensionless variable for a 3rd-order system. If you compare the inverse-Laplace transform for the 3rd-order chas. equation with the same xfr function for the 2nd order system, i.e. without the extra (s + αω
n) term, you would get a similar time response to a delta function input except for a modified coefficient in front of the sine term, plus a second, non-sinusoidal, term. The second term decays as exp(-αω
nt) whereas the sinusoidal part decays as exp(-ζω
nt), same as for the 2nd-order system. The argument of the sine is the same for both 2nd and 3rd order systems
= (ω
n√(1 - ζ
2)t + ψ).
And the phase angle ψ(3rd order) = ψ(2nd order) - a term including α.
So the bottom-line answer is that the two systems behave somewhat similarly if for the 3rd order system you retain the 2nd order expression multiplied by (s + αω
n).
The complete time response expression is a mess to write out & I'm not going to do it here, with or without the extra (s + αω
n) in the chas. equation. I suggest you get hold of a very extensive Laplace transform table which includes the time responses to both cases.