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An air capacitor is made from two flat parallel plates \(1.50 \mathrm{~mm}\) apart. The magnitude of charge on each plate is \(0.0180 \mu \mathrm{C}\) when the potential difference is \(200 \mathrm{~V}\). (a) What is the capacitance? (b) What is the area of each plate? (c) What maximum voltage can be applied without dielectric breakdown? (Dielectric breakdown for air occurs at an electric-field strength of \(3.0 \times 10^{6} \mathrm{~V} / \mathrm{m} .\) ) (d) When the charge is \(0.0180 \mu \mathrm{C},\) what total energy is stored?

Short Answer

Expert verified
The capacitance is approximately 90 pF. The area of each plate is approximately 0.202 m^2. The maximum voltage you can apply without dielectric breakdown is approximately 4.5 kV. The total energy stored is approximately 1.8 μJ.

Step by step solution

01

Determine the Capacitance

To get the capacitance \(C\), use the formula \(C = Q / V\), where \(Q\) is the charge (0.0180 μC converted to C) and \(V\) is the voltage (200 V). Find \(C\) accordingly.
02

Determine the Area of Each Plate

Determine the area \(A\) of each plate using the formula \(C = \epsilon A / d\), where \(\epsilon\) is the permittivity of free space (\(8.85 x 10^{-12} F/m\)), \(C\) is the capacitance (determined from step 1), and \(d\) is the plate separation distance (1.5 mm converted to m). Extract \(A\) by rearranging the equation.
03

Determine Maximum Voltage

Find the maximum voltage \(V_{max}\) that can be applied without dielectric breakdown using the formula \(E = V/d\), where \(E\) is the electric field strength (3.0 x 10^6 V/m) and \(d\) is the plate separation distance (1.5 mm converted to m). Rearrange the equation to solve for \(V_{max}\).
04

Determine Total Energy Stored

To find the total energy \(U\) stored when the charge is 0.0180 μC, use the formula \(U = 0.5 Q V\), where \(Q\) is the charge (0.0180 μC converted to C) and \(V\) is the voltage (200 V). Calculate \(U\) accordingly.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Capacitance Formula
Understanding the capacitance of a capacitor is fundamental in electronics. Capacitance, denoted by the symbol 'C', is a measure of a capacitor's ability to store charge per unit voltage. The basic formula for capacitance is \( C = \frac{Q}{V} \) where \( Q \) is the charge stored in coulombs, and \( V \) is the voltage across the capacitor in volts. In the context of the exercise, calculating the capacitance involves taking the stored charge on the capacitor plates and dividing it by the potential difference between them. This formula is significant because it links charge storage directly with the potential difference, which is a driving factor for the movement of charge in circuits.

Remember that in practice, real capacitors have a maximum capacitance which they should not exceed to function properly. Exceeding this can lead to capacitor malfunction or damage, reflecting the importance of correctly calculating and understanding capacitance.
Electric Field Strength
The electric field strength is a concept that relates to the force experienced by a positive test charge in the vicinity of other charges. It is represented by the symbol \( E \) and essentially tells us the intensity of the electric field at a point. The strength of this field in a capacitor is uniform between the plates and can be calculated using the formula \( E = \frac{V}{d} \) where \( V \) is the potential difference across the capacitor plates and \( d \) is the separation between them.

The electric field strength is a key player in determining how a capacitor will behave when subjected to a voltage. It influences the movement of electrons and hence the overall charge storage. If the electric field strength exceeds a certain threshold — known as dielectric breakdown — it can cause serious damage to the capacitor or the surrounding components.
Dielectric Breakdown
Dielectric breakdown is essentially the capacitor's worst nightmare. It is a failure mode which occurs when the electric field within a capacitor becomes too strong, causing the insulating material (in this case, air) to become conductive. For air, this breakdown strength is typically \( 3.0 \times 10^{6} \mathrm{~V/m} \).

When you calculate the maximum voltage that can be safely applied to the capacitor (as in the exercise), you are ensuring that the electric field strength does not exceed this critical threshold. If the voltage is too high, the insulating properties of the dielectric are compromised, leading to an uncontrolled discharge and possible damage. Calculating the maximum voltage — or staying below the breakdown voltage — is thus crucial for the safe operation of capacitors.
Energy Stored in a Capacitor
Capacitors not only store charge but also store energy in the form of an electric field between their plates. This energy can be calculated with the formula \( U = \frac{1}{2} Q V \) where \( U \) stands for the stored energy in joules, \( Q \) is the charge in coulombs, and \( V \) is the voltage in volts. In this scenario, when the charge is \(0.0180 \mu C\) and the voltage is 200 V, applying this formula gives us the total energy stored in the capacitor.

Understanding this concept is essential for various applications, including power systems that use capacitors for energy storage and electronics, where capacitors can provide bursts of energy. The energy stored can also lead to hazardous situations if not handled properly, as it can cause electric shocks or damage when discharged suddenly. Therefore, accurately calculating this energy is as crucial for functionality as it is for safety.

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Most popular questions from this chapter

A capacitor is formed from two concentric spherical conducting shells separated by vacuum. The inner sphere has radius \(12.5 \mathrm{~cm},\) and the outer sphere has radius \(14.8 \mathrm{~cm} .\) A potential difference of \(120 \mathrm{~V}\) is applied to the capacitor. (a) What is the energy density at \(r=12.6 \mathrm{~cm}\), just outside the inner sphere? (b) What is the energy density at \(r=14.7 \mathrm{~cm},\) just inside the outer sphere? (c) For a parallel-plate capacitor the energy density is uniform in the region between the plates, except near the edges of the plates. Is this also true for a spherical capacitor?

A \(5.00 \mu \mathrm{F}\) parallel-plate capacitor is connected to a \(12.0 \mathrm{~V}\) battery. After the capacitor is fully charged, the battery is disconnected without loss of any of the charge on the plates. (a) A voltmeter is connected across the two plates without discharging them. What does it read? (b) What would the voltmeter read if (i) the plate separation were doubled; (ii) the radius of each plate were doubled but their separation was unchanged?

CP Dielectric elastomers are used to create voltage-dependent capacitors. These elastomers contract when subject to the stresses induced by Coulomb forces between capacitor plates. Consider a pair of parallel plates with area \(A\) separated by distance \(d_{0}\) when no voltage is applied. A material with dielectric constant \(K\) and Young's modulus \(Y\) fills the space between the plates. (a) What compressive force is applied to the dielectric when the plates have opposite charges \(Q\) and \(-Q ?\) (b) The distance between the plates is \(d=d_{0}-s Q^{2},\) where \(s\) is a squeezing coefficient. Determine \(s\) in terms of the parameters specified. (c) A capacitor of this sort has plate area \(1.00 \mathrm{~cm}^{2}\) and noncharged separation distance \(d_{0}=0.400 \mathrm{~mm}\). The plates are separated by a silicone dielectric elastomer with dielectric constant \(K=3.00\) and Young's modulus \(0.0100 \mathrm{GPa}\). What is the squeezing coefficient in this case? (d) If each plate has charge of magnitude \(0.700 \mu \mathrm{C}\), what is the applied voltage? (e) What new voltage would double the amount of charge on the plates?

A fuel gauge uses a capacitor to determine the height of the fuel in a tank. The effective dielectric con- stant \(K_{\text {eff }}\) changes from a value of 1 when the tank is empty to a value of \(K\), the dielectric constant of the fuel, when the tank is full. The appropriate electronic circuitry can determine the effective dielectric constant of the combined air and fuel between the capacitor plates. Each of the two rectangular plates has a width \(w\) and a length \(L\) (Fig. \(\mathbf{P 2 4 . 6 6}\) ). The height of the fuel between the plates is \(h\). You can ignore any fringing effects. (a) Derive an expression for \(K_{\text {eff }}\) as a function of \(h\). (b) What is the effective dielectric constant for a tank \(\frac{1}{4}\) full, \(\frac{1}{2}\) full, and \(\frac{3}{4}\) full if the fuel is gasoline \((K=1.95) ?\) (c) Repeat part (b) for methanol \((K=33.0)\). (d) For which fuel is this fuel gauge more practical?

A cylindrical capacitor has an inner conductor of radius \(2.2 \mathrm{~mm}\) and an outer conductor of radius \(3.5 \mathrm{~mm} .\) The two conductors are separated by vacuum, and the entire capacitor is \(2.8 \mathrm{~m}\) long. (a) What is the capacitance per unit length? (b) The potential of the inner conductor is \(350 \mathrm{mV}\) higher than that of the outer conductor. Find the charge (magnitude and sign) on both conductors.

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