{{page>wiki:headers:hheader}} =====Approximating the N-th Normal Mode Frequency for an N-chain Oscillator (10 minutes)===== * If an N-chain oscillator is oscillating at the N-th normal mode in the first Burilloun zone (that is, when the wavelength of the envelope function is $k=\frac{\pi}{a}$), the frequency of oscillation can be reasonably approximated using the equation of motion for a particle in the system. {{courses:lecture:pplec:pplecnmodefig1.png|}} * The key approximation for this calculation is that the displacement of each molecule in the oscillator is equal in magnitude. Using this approximation, the equation of motion for a particular particle becomes $$m\ddot{x}=-2\kappa x \; - \; 2\kappa x \; \; . $$ Assuming that the equation describing the particle's motion has the form $$x(t)=Ae^{i \omega t} \; \; , $$ this equation can be inserted into the equation of motion to find that $$\omega=\sqrt{\frac{4\kappa}{m}} \; \; . $$ //Have the students test this approximation using the "One Dimensional Oscillator Chain" program. This exercise works quite well as an extension in concluding the [[..:..:..:courses:activities:ppact:ppperiodiclab1|Coupled Oscillators and the Monatomic Chain Lab]].// {{page>wiki:footers:courses:ppfooter}}