Using the Angular Frequency to Solve a Differential Equation

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Homework Statement


Im somewhat unsure of what the result i have derived is exactly. I know the angular frequency should be
[tex]\omega = \sqrt{\frac{k}{m} - \frac{{b}^{2}}{4{m}^{2}}}[/tex]


The Attempt at a Solution


[tex]m\frac{{d}^{2}x}{d{t}^{2}} = -kx -b\frac{dx}{dt}[/tex]
Sub in [tex]\omega = \sqrt{\frac{k}{m}}[/tex]
Do [tex]x = {e}^{\lambda t}[/tex]
x' = ...
x''=...

[tex]{e}^{\lambda t}({\lambda}^{2} + \lambda \frac{b}{m} + {\omega}^{2}) = 0[/tex]
[tex]\lambda = -\frac{b}{2m} \pm \sqrt{\frac{{b}^{2}}{{4m}^{2}} - 4\frac{{\omega}^{2}}{4}}[/tex]

However, i thought
[tex]\omega = \sqrt{\frac{k}{m} - \frac{{b}^{2}}{4{m}^{2}}}[/tex]

Are these results related as i cannot quite put my tongue on how to get this result from the [tex]\lambda[/tex] result (And I am not entirely sure what [tex]\lambda[/tex] representes in real terms)

Thanks!
 
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Substitute something like a = k/m (k/m isn't the angular frequency in a damped system.), and let x = exp(omega t) instead of exp(lambda t).

If you get stumped when you solve for omega, evaluate the sign of the argument under the square root.