Solution to Set 5: Difference between revisions

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<math>u_m(t)=e^{i\omega t} u_m \;</math>
<math>u_m(t)=e^{i\omega t} u_m \;</math>


<font color="blue">What does the subscript m stand for? Modes? [[User:KimberlyWynne|KimberlyWynne]] 03:36, 2 March 2009 (EST)</font>
<font color="blue">What does the subscript m stand for? Modes? What are modes? - [[User:KimberlyWynne|KimberlyWynne]] 03:36, 2 March 2009 (EST)</font>


<math>\Rightarrow -m \omega ^2 \vec{u} = - k \mathbf{M} \vec{u} \;</math>
<math>\Rightarrow -m \omega ^2 \vec{u} = - k \mathbf{M} \vec{u} \;</math>
Line 44: Line 44:
<math>\Rightarrow -m \omega ^2 \vec{u} = - k [2 - e^{ik \alpha} - e^{-ik \alpha}] \;</math>
<math>\Rightarrow -m \omega ^2 \vec{u} = - k [2 - e^{ik \alpha} - e^{-ik \alpha}] \;</math>


<math>\omega (k) = 2 \sqrt{ \frac{k}{m} } |sin(ka)|</math>
Derive and get:
 
<math>\Rightarrow \omega (k) = 2 \sqrt{ \frac{k}{m} } |sin(ka)|</math>
[[Image:Dispersionrelation.jpg]]
[[Image:Dispersionrelation.jpg]]



Revision as of 04:45, 2 March 2009

I have no idea what I'm doing - KimberlyWynne 03:11, 2 March 2009 (EST)

Diatomic harmonic chain

Problem 1

Given:

  • a chain of atoms
  • with alternating masses and
  • connected with elastic springs with constant
  • moving only in the x-direction

Chainatoms.jpg

Derive the dispersion relation for this chain

  • Index for acoustic branch
  • Index for optical branch

Potential Energy

Eigenvector Value for modes

What does the subscript m stand for? Modes? What are modes? - KimberlyWynne 03:36, 2 March 2009 (EST)

Band Matrix

where

Derive and get:

Dispersionrelation.jpg

Problem 2

Determine the speed of sound for this chain. What is the lowest frequency of long-wavelength sound corresponding to the optical branch?

From my lecture notes:

where = speed of sound

Problem 3

Sketch the motion of the atoms corresponding to the edge of the Brillouin zone, both for the optical and the acoustic branch.

Problem 4

Determine the Debye temperature for this system, and determine the form of the specific heat in the limits of high and low temperatures.

Problem 5

Consider low temperatures () and determine the wavelength of the most abundant phonons (Hint: note the analogy with Wien's Law!)