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A parallel plate capacitor with vacuum between the plates has a capacitance of \(3.669 \mu \mathrm{F}\). A dielectric material with \(\kappa=3.533\) is placed between the plates, completely filling the volume between them. The capacitor is then connected to a battery that maintains a potential difference \(V\) across the plates. The dielectric material is pulled out of the capacitor, which requires \(7.389 \cdot 10^{-4} \mathrm{~J}\) of work. What is the potential difference, \(V ?\)

Short Answer

Expert verified
Answer: The potential difference across the parallel plate capacitor is approximately 1.260 V.

Step by step solution

01

Calculate Capacitance C2 after inserting the dielectric

To find C2, we can use the formula C2 = κC1, where κ is the dielectric constant. C2 = (3.533)(3.669 * 10^{-6} F) = 12.954 * 10^{-6} F
02

Find the initial and final energies stored in the capacitor

We can use the formula U = (1/2) * C * V^2 to find the energy stored before and after inserting the dielectric material. Also, we know that the potential difference V does not change when a dielectric is inserted. U1 = (1/2) * C1 * V^2 U2 = (1/2) * C2 * V^2
03

Calculate the change in energy

The difference in energy between the initial and final states (ΔU) is equal to the work required to remove the dielectric (W). ΔU = U2 - U1 = W
04

Express the potential difference V in terms of given values

We can express the potential difference V by substituting the expressions for U1 and U2 from Step 2 and ΔU from Step 3. (1/2) * C2 * V^2 - (1/2) * C1 * V^2 = W (1/2) * (C2 - C1) * V^2 = W V^2 = (2 * W) / (C2 - C1)
05

Find the potential difference V

Now, we can substitute the values for W, C1, and C2 in the expression for V^2, and finally find V. V^2 = 2 * (7.389 * 10^{-4} J) / (12.954 * 10^{-6} F - 3.669 * 10^{-6} F) V^2 = (2 * 7.389 * 10^{-4}) / (9.285 * 10^{-6}) V = sqrt(1.587443) V ≈ 1.260 V The potential difference across the parallel plate capacitor is approximately 1.260 V.

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Most popular questions from this chapter

Two capacitors, with capacitances \(C_{1}\) and \(C_{2},\) are connected in series. A potential difference, \(V_{0}\), is applied across the combination of capacitors. Find the potential differences \(V_{1}\) and \(V_{2}\) across the individual capacitors, in terms of \(V_{0}, C_{1},\) and \(C_{2}\)

A capacitor consists of two parallel plates, but one of them can move relative to the other as shown in the figure. Air fills the space between the plates, and the capacitance is \(32.0 \mathrm{pF}\) when the separation between plates is \(d=0.500 \mathrm{~cm}\) a) A battery supplying a potential difference \(V=9.00 \mathrm{~V}\) is connected to the plates. What is the charge distribution, \(\sigma,\) on the left plate? What are the capacitance, \(C^{\prime},\) and the charge distribution, \(\sigma^{\prime},\) when \(d\) is changed to \(0.250 \mathrm{~cm} ?\) b) With \(d=0.500 \mathrm{~cm}\), the battery is disconnected from the plates. The plates are then moved so that \(d=0.250 \mathrm{~cm}\) What is the potential difference \(V^{\prime}\) between the plates?

Two capacitors with capacitances \(C_{1}\) and \(C_{2}\) are connected in series. Show that, no matter what the values of \(C_{1}\) and \(C_{2}\) are, the equivalent capacitance is always less than the smaller of the two capacitances.

An isolated solid spherical conductor of radius \(5.00 \mathrm{~cm}\) is surrounded by dry air. It is given a charge and acquires potential \(V\), with the potential at infinity assumed to be zero. a) Calculate the maximum magnitude \(V\) can have. b) Explain clearly and concisely why there is a maximum.

Calculate the maximum surface charge distribution that can be maintained on any surface surrounded by dry air.

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