Finding the general solution of this ODE

[Benny]

Hi can someone help me out with the following question?

Q. The differential equation for unforced under-damped oscillatory motion can be written \mathop x\limits^{..} + 2p\mathop x\limits^. + \omega ^2 x = 0 where the constants p and omega satisfy 0 < p < \omega.

Find the general solution of this differential equation, and show that this solution can be expressed in the form x = {\mathop{\rm Re}\nolimits} ^{ - pt} \cos \left( {\sqrt {\omega ^2 - p^2 } t - \alpha } \right) where R and alpha are constants.

<br /> x\left( t \right) = e^{ - pt} \left( {c_1 \cos \left( {t\sqrt {p^2 - \omega ^2 } } \right) + c_2 \sin \left( {t\sqrt {p^2 - \omega ^2 } } \right)} \right)<br /> by using 0 < p < omega.

As can be seen I haven't been able to get too far. I can't think of a way to get to the answer. Can someone please help me out?

 

[HallsofIvy]

Yes, the characteristic equation is r²+ 2pr+ &omega;= 0 (You have &omega;² in the differential equation but your solution seems to be for &omega; only) and the solutions to that are -p\pm\sqrt{p^2-\omega^2}= -p\pm\sqrt{\omega^2-p^}i.
Yes, the general solution to the differential equation is
e^{-pt}\left(C_1 Cos(\sqrt{\omega^2-p^2}t)+C_2 Sin(\sqrt{\omega^2-p^2}t\right).

Now, all you want to do is show that that can be expressed as a single cosine.

Use the trig identity: Cos(a+ b)= Cos(a)Cos(b)- Sin(a)Sin(b).

Obviously, you want b= \sqrt{\omega^2-p^2}. You will need to find a such that Cos(a)= C₁, Sin(a)= C₂. Obviously that can't happen unless the sum of their squares is equal to 1: that's where R comes in: What is the sum of the squares now?