Dielectrics: An Atomic View — Question 8

Section 25-6 · Physics pages 4126–4127

Question 8 Random dipoles have zero mean polarization but a nonzero finite-sample fluctuation N independent isotropically oriented permanent dipoles of magnitude p occupy volume V. At zero field, ⟨pz⟩= 0 and ⟨p2 z⟩= p2/3. Let n=N/V. Schematic; labels, not drawing lengths, specify the data. (a) Find the mean and variance of the total z-directed dipole moment. (b) Find the root-mean-square polarization component and its ratio to the saturation magnitude np.
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Question 8 - Solution Random dipoles have zero mean polarization but a nonzero finite-sample fluctuation (a) Method and calculation Mz = N ∑ i=1 pz,i, ⟨Mz⟩= 0. ⟨M2 z ⟩= ∑ i ⟨p2 z,i⟩+ ∑ i̸=j ⟨pz,i⟩⟨pz,j⟩= Np2/3. (b) Interpretation and further calculation Pz,rms = p √ N/3 V . Pz,rms np = 1 √ 3N . Physical check Zero ensemble mean does not imply zero moment in every microscopic snapshot; relative fluctuations shrink as inverse square root of sample size.

Question 8

Random dipoles have zero mean polarization but a nonzero finite-sample fluctuation

N independent isotropically oriented permanent dipoles of magnitude p occupy volume 𝒱\mathcal V. At zero field, ⟨pz⟩=0\langle p_z\rangle=0 and ⟨pz2⟩=p2/3\langle p_z^2\rangle=p^2/3. Let n=N/𝒱\mathcal V.

Diagram shown in the original SVG worksheet.

  1. Find the mean and variance of the total z-directed dipole moment.

  2. Find the root-mean-square polarization component and its ratio to the saturation magnitude np.

Question 8 - Solution

Random dipoles have zero mean polarization but a nonzero finite-sample fluctuation

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Mz=∑i=1Npz,i,⟨Mz⟩=0.M_z=\sum_{i=1}^Np_{z,i},\quad\langle M_z\rangle=0.⟨Mz2⟩=∑i⟨pz,i2⟩+∑i≠j⟨pz,i⟩⟨pz,j⟩=Np2/3.\langle M_z^2\rangle=\sum_i\langle p_{z,i}^2\rangle+\sum_{i\ne j}\langle p_{z,i}\rangle\langle p_{z,j}\rangle=Np^2/3.

(b) Interpretation and further calculation

Pz,rms=pN/3𝒱.P_{z,\mathrm{rms}}=\frac{p\sqrt{N/3}}{\mathcal V}.Pz,rmsnp=13N.\frac{P_{z,\mathrm{rms}}}{np}=\frac1{\sqrt{3N}}.

Physical check

Zero ensemble mean does not imply zero moment in every microscopic snapshot; relative fluctuations shrink as inverse square root of sample size.