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

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The analysis of critically damped motion was incorrect due to the assumption of a complex solution, which is not applicable in this case. For critically damped or overdamped oscillators, the solutions are real rather than complex. The correct approach involves assuming an exponential solution and deriving the characteristic equation, which leads to real roots for critically damped systems. The general solution for critical damping includes a linear combination of exponentials with a double root. Understanding these principles is essential for correctly solving differential equations related to motion.
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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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