alfredblase
- 228
- 0
Show that
q_{c}(t)=\frac{1}{\sinh \omega \tau} }[ q' \sinh{\omega(t''-t)} + q'' \sinh{\omega(t-t')} ]
is the solution to the classical equation of motion for the harmonic oscillator
\ddot {q}_{c}(t)-\omega^{2}q_{c}(t)=0
where q_{c}(t) is the position vector, \tau = t'' - t', q_{c}(t')=q', q_{c}(t'')=q'' and \ddot {q}_{c}(t) is the double time derivative of q_{c}(t)
I can differentiate q_{c}(t) twice with respect to time easily enough to show that that the first equation is a solution to the equation of motion but there are many functions that satisfy this.
How do I show that it's the solution?
I've tried solving the equation of motion directly but I can't find any way to solve it so that I end up with q_{c}(t) as a funciton of t, t', t'', q' and q''. (For example the way everyone is usually taught to solve it, you simply end up with a sin function of t multiplied by an amplitude..)
Any help/suggestions would be very much appreciated. Thank you for taking the time to read this :)
q_{c}(t)=\frac{1}{\sinh \omega \tau} }[ q' \sinh{\omega(t''-t)} + q'' \sinh{\omega(t-t')} ]
is the solution to the classical equation of motion for the harmonic oscillator
\ddot {q}_{c}(t)-\omega^{2}q_{c}(t)=0
where q_{c}(t) is the position vector, \tau = t'' - t', q_{c}(t')=q', q_{c}(t'')=q'' and \ddot {q}_{c}(t) is the double time derivative of q_{c}(t)
I can differentiate q_{c}(t) twice with respect to time easily enough to show that that the first equation is a solution to the equation of motion but there are many functions that satisfy this.
How do I show that it's the solution?
I've tried solving the equation of motion directly but I can't find any way to solve it so that I end up with q_{c}(t) as a funciton of t, t', t'', q' and q''. (For example the way everyone is usually taught to solve it, you simply end up with a sin function of t multiplied by an amplitude..)
Any help/suggestions would be very much appreciated. Thank you for taking the time to read this :)
Last edited: