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Math 6420 • PDE

Fall 2002 • Question 2

Consider a linear chain of \(2N\) atoms with the same spacing \(a\) and force constant \(\beta \) but of two different masses \(m,M\), \(M>m\), placed alternately. Label the light atoms by even integers \(2n\), \(n=0,\ldots ,N-1\) and the heavy atoms by odd integers \(2n-1\), \(n=1,\ldots ,N\). Denoting their displacements from equilibrium by the variables \(U_{2n}\) and \(V_{2n-1}\), Newton’s law of motion gives \[ \begin {aligned} m\ddot {U}_{2n} &= \beta [V_{2n-1}+V_{2n+1}-2U_{2n}],\\ M\ddot {V}_{2n-1} &= \beta [U_{2n}+U_{2n-2}-2V_{2n-1}]. \end {aligned} \] Determine the modes of vibration of the system and sketch the resulting pair of dispersion curves. [Assume periodic boundary conditions \(U_0=U_{2N}\) and \(V_1=V_{2N+1}\).]

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Consider a linear chain of \(2N\) atoms with the same spacing \(a\) and force constant
\(\beta\) but of two different masses \(m,M\), \(M>m\), placed alternately. Label the light
atoms by even integers \(2n\), \(n=0,\ldots,N-1\) and the heavy atoms by odd integers
\(2n-1\), \(n=1,\ldots,N\). Denoting their displacements from equilibrium by the variables
\(U_{2n}\) and \(V_{2n-1}\), Newton's law of motion gives
\[
\begin{aligned}
m\ddot{U}_{2n} &= \beta[V_{2n-1}+V_{2n+1}-2U_{2n}],\\
M\ddot{V}_{2n-1} &= \beta[U_{2n}+U_{2n-2}-2V_{2n-1}].
\end{aligned}
\]
Determine the modes of vibration of the system and sketch the resulting pair of dispersion
curves. [Assume periodic boundary conditions \(U_0=U_{2N}\) and \(V_1=V_{2N+1}\).]