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Physics LibreTexts

5.14: Mixed Dielectrics

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This section addresses the question: If there are two or more dielectric media between the plates of a capacitor, with different permittivities, are the electric fields in the two media different, or are they the same? The answer depends on

  1. Whether by “electric field” you mean E or D;
  2. The disposition of the media between the plates – i.e. whether the two dielectrics are in series or in parallel.

Let us first suppose that two media are in series (Figure V.16).

V.16.png

\text{FIGURE V.16}

Our capacitor has two dielectrics in series, the first one of thickness d_1 and permittivity \epsilon_1 and the second one of thickness d_2 and permittivity \epsilon_2. As always, the thicknesses of the dielectrics are supposed to be small so that the fields within them are uniform. This is effectively two capacitors in series, of capacitances \epsilon_1A/d_1 \text{ and }\epsilon_2A/d_2. The total capacitance is therefore

C=\frac{\epsilon_1\epsilon_2A}{\epsilon_2d_1+\epsilon_1d_2}.\label{5.14.1}

Let us imagine that the potential difference across the plates is V_0. Specifically, we’ll suppose the potential of the lower plate is zero and the potential of the upper plate is V_0. The charge Q held by the capacitor (positive on one plate, negative on the other) is just given by Q = CV_0, and hence the surface charge density \sigma is CV_0/A. Gauss’s law is that the total D-flux arising from a charge is equal to the charge, so that in this geometry D = \sigma, and this is not altered by the nature of the dielectric materials between the plates. Thus, in this capacitor, D = CV_0/A = Q/A in both media. Thus D is continuous across the boundary.

Then by application of D = \epsilon E to each of the media, we find that the E-fields in the two media are E_1=Q/(\epsilon_1A) and E_2=Q/(\epsilon_2A), the E-field (and hence the potential gradient) being larger in the medium with the smaller permittivity.

The potential V at the media boundary is given by V/d_2=E_2. Combining this with our expression for E_2, and Q = CVand Equation \ref{5.14.1}, we find for the boundary potential:

V=\frac{\epsilon_1d_2}{\epsilon_2d_1+\epsilon_1d_2}V_0.\label{5.14.2}

Let us now suppose that two media are in parallel (Figure V.17).

V.17.png

\text{FIGURE V.17}

This time, we have two dielectrics, each of thickness d, but one has area A_1 and permittivity \epsilon_1 while the other has area A_2 and permittivity \epsilon_2. This is just two capacitors in parallel, and the total capacitance is

C=\frac{\epsilon_1A_1}{d}+\frac{\epsilon_2A_2}{d}\label{5.14.3}

The E-field is just the potential gradient, and this is independent of any medium between the plates, so that E = V/d. in each of the two dielectrics. After that, we have simply that D_1=\epsilon_1E \text{ and }D_2=\epsilon_2E. The charge density on the plates is given by Gauss’s law as \sigma = D, so that, if \epsilon_1 < \epsilon_2, the charge density on the left hand portion of each plate is less than on the right hand portion – although the potential is the same throughout each plate. (The surface of a metal is always an equipotential surface.) The two different charge densities on each plate is a result of the different polarizations of the two dielectrics – something that will be more readily understood a little later in this chapter when we deal with media polarization.

We have established that:

  1. The component of \textbf{D} perpendicular to a boundary is continuous;
  2. The component of \textbf{E} parallel to a boundary is continuous.

In Figure V.18 we are looking at the D-field and at the E-field as it crosses a boundary in which \epsilon_1 < \epsilon_2. Note that D_y and E_xare the same on either side of the boundary. This results in:

\frac{\tan \theta_1}{\tan \theta_2}=\frac{\epsilon_1}{\epsilon_2}.\label{5.14.4}

V.18.png

\text{FIGURE V.18}


This page titled 5.14: Mixed Dielectrics is shared under a CC BY-NC 4.0 license and was authored, remixed, and/or curated by Jeremy Tatum via source content that was edited to the style and standards of the LibreTexts platform.

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