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A parallel-plate capacitor is filled with a nonuniform dielectric characterized by \(\epsilon_{r}=2+2 \times 10^{6} x^{2}\), where \(x\) is the distance from one plate in meters. If \(S=0.02 \mathrm{~m}^{2}\) and \(d=1 \mathrm{~mm}\), find \(C\).

Short Answer

Expert verified
Based on the given problem of a parallel-plate capacitor filled with a nonuniform dielectric, we have calculated the capacitance of the capacitor to be approximately \(3.54 \times 10^{-11} \mathrm{F}\).

Step by step solution

01

Calculate the relative permittivity

Given, the relative permittivity is defined by the formula \(\epsilon_{r} = 2 + 2 \times 10^{6}x^{2}\). The total permittivity, \(\epsilon\), can be found by multiplying the relative permittivity by the vacuum permittivity, \(\epsilon_{0}\). So, \(\epsilon = \epsilon_{0} \epsilon_{r} = \epsilon_{0}(2 + 2 \times 10^{6}x^{2})\).
02

Calculate capacitance for infinitesimally small distances

We'll now find the capacitance for an infinitesimally small distance \(dx\) within the capacitor. Using the formula \(C = \frac{\epsilon A}{d}\), the capacitance for a small distance \(dx\) will be \(dC = \frac{\epsilon S}{dx} = \frac{\epsilon_{0}(2 + 2 \times 10^{6}x^{2})S}{dx}\).
03

Integrate to find the total capacitance

To find the total capacitance of the capacitor, we'll integrate the \(dC\) expression over the entire distance between the plates, from 0 to \(d=1\) mm, or 0 to \(10^{-3}\) meters. This will give us: \(C = \int_{0}^{10^{-3}} \frac{\epsilon_{0}(2 + 2 \times 10^6 x^2)S}{dx}\).
04

Perform the integration

To perform the integration, we can first distribute the constants outside of the integral: \(C = \epsilon_{0}S\int_{0}^{10^{-3}} \frac{2 + 2 \times 10^{6}x^{2}}{dx}\). Now, integrating with respect to \(x\), we get: \(C = \epsilon_{0}S\left[2x + \frac{2}{3} \times 10^{6}x^{3}\right]_{0}^{10^{-3}}\).
05

Evaluate the integral

Evaluating the integral at the limits of 0 and \(10^{-3}\), we get: \(C = \epsilon_{0}S\left[2(10^{-3}) + \frac{2}{3} \times 10^{6}(10^{-3})^{3}\right]\).
06

Calculate the capacitance

Using the value of vacuum permittivity, \(\epsilon_{0} = 8.854 \times 10^{-12} \mathrm{F/m}\), and the given plate area, \(S = 0.02 \mathrm{m^2}\), we can calculate the capacitance: \(C = (8.854 \times 10^{-12})(0.02)\left[2(10^{-3}) + \frac{2}{3} \times 10^{6}(10^{-3})^{3}\right]\). After evaluating this expression, we find that the capacitance of the parallel-plate capacitor is approximately \(3.54 \times 10^{-11} \mathrm{F}\).

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Most popular questions from this chapter

A parallel-plate capacitor has plates located at \(z=0\) and \(z=d\). The region between plates is filled with a material that contains volume charge of uniform density \(\rho_{0} \mathrm{C} / \mathrm{m}^{3}\) and has permittivity \(\epsilon\). Both plates are held at ground potential. ( \(a\) ) Determine the potential field between plates. (b) Determine the electric field intensity \(\mathbf{E}\) between plates. \((c)\) Repeat parts \((a)\) and \((b)\) for the case of the plate at \(z=d\) raised to potential \(V_{0}\), with the \(z=0\) plate grounded.

Capacitors tend to be more expensive as their capacitance and maximum voltage \(V_{\max }\) increase. The voltage \(V_{\max }\) is limited by the field strength at which the dielectric breaks down, \(E_{B D}\). Which of these dielectrics will give the largest \(C V_{\max }\) product for equal plate areas? \((a)\) Air: \(\epsilon_{r}=1\), \(E_{B D}=3 \mathrm{MV} / \mathrm{m} .(b)\) Barium titanate: \(\epsilon_{r}=1200, E_{B D}=3 \mathrm{MV} / \mathrm{m} .(c)\) Silicon dioxide: \(\epsilon_{r}=3.78, E_{B D}=16 \mathrm{MV} / \mathrm{m} .(d)\) Polyethylene: \(\epsilon_{r}=2.26, E_{B D}=\) \(4.7 \mathrm{MV} / \mathrm{m} .\)

In free space, let \(\rho_{v}=200 \epsilon_{0} / r^{2.4}\). (a) Use Poisson's equation to find \(V(r)\) if it is assumed that \(r^{2} E_{r} \rightarrow 0\) when \(r \rightarrow 0\), and also that \(V \rightarrow 0\) as \(r \rightarrow \infty\). (b) Now find \(V(r)\) by using Gauss's law and a line integral.

An air-filled parallel-plate capacitor with plate separation \(d\) and plate area \(A\) is connected to a battery that applies a voltage \(V_{0}\) between plates. With the battery left connected, the plates are moved apart to a distance of \(10 d\). Determine by what factor each of the following quantities changes: \((a) V_{0} ;(b) C ;(c) E ;(d) D ;(e) Q ;(f) \rho_{S} ;(g) W_{E}\)

Given the spherically symmetric potential field in free space, \(V=V_{0} e^{-r / a}\), find. (a) \(\rho_{v}\) at \(r=a ;(b)\) the electric field at \(r=a ;(c)\) the total charge.

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