Why did my analysis of critically damped motion lead to the wrong solution?

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SUMMARY

The analysis of critically damped motion using the differential equation x'' + y*x' + ω₀²x = 0 was incorrectly approached by assuming a complex solution z = A*e^(i(wt+a)). The correct method involves recognizing that critically damped and overdamped oscillators yield real solutions, not complex ones. The characteristic equation derived from substituting an exponential solution into the ODE leads to real roots for critical damping, resulting in the general solution of the form e^(λt)(c₁ + c₂t) when a double root occurs.

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Why is my analysis of critically damped motion wrong?
x'' + y*x' + wo²x = 0

Choosing a complex number z as z = A*e^i(wt+a) and putting on the equation calling x as the real part of Z

w = ( i*y +- (4wo²-y²)^(1/2) )/2 (bhaskara)

2wo = y (critical)

w = iy/2

z = A*e^i(ity/2 + a)
z = A*e^(-yt/2 + a)
x = A*e^(-yt/2)*cos(a)
 
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In the rolling of this question, i think the wrong step i did was adopt z as i adopted, but, if is this, raised up another question:
I am still a beginner dealing with this type of solution of differential equation by complex, so, how would i know the right z i need to assume before starting the mathematical steps?
 
LCSphysicist said:
In the rolling of this question, i think the wrong step i did was adopt z as i adopted, but, if is this, raised up another question:
I am still a beginner dealing with this type of solution of differential equation by complex, so, how would i know the right z i need to assume before starting the mathematical steps?
In case of critically damped or overdamped oscillators, the solution is not complex.
Read about the solutions of linear, constant- coefficient homogeneous ODE-s. (https://www.math24.net/second-order-linear-homogeneous-differential-equations-constant-coefficients/ , for example)
Usually, we start solving such equations by assuming the solution in exponential form ##y=e^{\lambda t}##, substituting back into the ODE and getting the characteristic equation for lambda, a quadratic equation, which has either complex roots (underdamped oscillator) or two different real roots (overdamped oscillator) or a double root in case of critical damping.
While the general solution is linear combination of the different exponentials, the solution is ##e^{\lambda t}(c_1+c_2t)## in case of double root, that is critical damping.
 
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