Electromagnetism and Polarisation question

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Homework Help Overview

The problem involves the effects of a uniform electric field on diamond, specifically focusing on induced polarization, dipole moments, and charge separation. It requires calculations related to the density of diamond, the number of carbon atoms per cubic meter, and the resultant polarization current density in an alternating electric field.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of the number of carbon atoms in diamond and the average induced dipole moment. There is a concern about the estimated separation of charges being too small compared to expected atomic radii. Questions arise regarding the assumptions made in the calculations and the implications of applying an external electric field.

Discussion Status

Some participants provide clarifications regarding the relationship between the average dipole moment and atomic dimensions, while others question the assumptions about the dipole's length in relation to atomic structure. The discussion appears to be productive, with participants exploring different interpretations of the results.

Contextual Notes

Participants note that the average dipole moment calculated does not correspond to typical atomic radii, suggesting a potential misunderstanding or miscalculation. The role of the external electric field in influencing charge behavior is also highlighted.

jazznaz
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Homework Statement



When a uniform electric field is applied to diamond, the induced dipole moment per unit volume (ie. polarisation) is [tex]P_{0} = 1.5 \times 10^{-7} \text{C m}^{-2}[/tex]. Given that the density of diamond is [tex]3500 \text{kg m}^{-3}[/tex], 1 kmole of diamond has a mass of 12kg. Avogadro's constant is [tex]6 \times 10^{26} \text{kmol}^{-1}[/tex], the atomic number of carbon is 6.

How many carbon atoms are there per cubic metre?
What is the average induced dipole moment?
Estimate the average separation of the +ve and -ve charges.
If [tex]P = P_{0} \sin \omega t[/tex] as a result of the alternating electric field, evaluate the peak value of the resultant polarisation current density, J, at a frequency of [tex]10^{12} \text{Hz}[/tex]

The Attempt at a Solution



First part,

[tex]\rho = \frac{m}{v} = 3500[/tex]

[tex]m = 3500[/tex]

[tex]m/0.012 = 291666.67 \text{moles}[/tex]

[tex]291666.67 \times 6 \times 10^{23} = 1.8 \times 10^{29} \text{atoms m}^{-3}[/tex]

Second part,

Average induced dipole moment is total polarisation divided by number of atoms,

[tex]= \frac{1.5 \times 10^{7}}{1.8 \times 10^{29}}= 8.3 \times 10^{-23} \text{C m}[/tex]

Third part,

Dipole moment is [tex]\vec{p} = q\vec{L}[/tex]

So [tex]L = \frac{p}{q} = \frac{8.3 \times 10^{-23}}{6 \times 1.6 \times 10^{-19}} = 8.6 \times 10^{-5} \text{m}[/tex]

Which strikes me as far too small to be an estimate of the atomic radius of a carbon atom in the diamond lattice. I can't see where I've gone wrong, maybe I've missed a subtlety in the question?

Any comments would be great, thanks...
 
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The avergare dipole moment is not the atomic radius of the atom. The value you obtained on the order of 10 microns is much larger than then atomic radii on the order of nanometers.
 
In this case, the dipole is between the carbon nuclei and the surrounding electron cloud, so I expected the dipole moment to be acting over a length similar to the atomic radius.
 
Keep in mind an external electric field is applied thereby applying a force to the charges.
 

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