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24.26. 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
(a) 9.0×10^{-11} F; (b) 1.53×10^{-2} m²; (c) 4500 V; (d) 1.8×10^{-6} J.

Step by step solution

01

Calculate Capacitance

To calculate the capacitance, we use the formula for capacitance in terms of charge and voltage: \[ C = \frac{Q}{V} \] where \( Q = 0.0180 \mu C \) and \( V = 200 V \). Convert \( Q \) to coulombs by multiplying by \( 1 \times 10^{-6} \) :\[ Q = 0.0180 \times 10^{-6} C = 1.8 \times 10^{-8} C \] Now substitute into the formula:\[ C = \frac{1.8 \times 10^{-8}}{200} = 9 \times 10^{-11} F \] Thus, the capacitance is \( 9.0 \times 10^{-11} F \).
02

Calculate the Plate Area

To find the area \( A \) of each plate, use the formula for the capacitance of a parallel plate capacitor:\[ C = \frac{\varepsilon_0 A}{d} \] where \( \varepsilon_0 = 8.85 \times 10^{-12} \, F/m \) is the permittivity of free space, and \( d = 1.5 \times 10^{-3} m \) is the distance between the plates. We already calculated \( C = 9 \times 10^{-11} F \).Rearrange the formula to solve for \( A \): \[ A = \frac{C \cdot d}{\varepsilon_0} = \frac{9 \times 10^{-11} \cdot 1.5 \times 10^{-3}}{8.85 \times 10^{-12}} \approx 1.53 \times 10^{-2} m^2 \]So, the area of each plate is \( 1.53 \times 10^{-2} m^2 \).
03

Calculate Maximum Voltage Without Breakdown

The maximum voltage \( V_{max} \) without causing dielectric breakdown can be calculated using the formula:\[ V_{max} = E_{break} \times d \] where \( E_{break} = 3.0 \times 10^6 \, V/m \) is the breakdown electric field strength. Use \( d = 1.5 \times 10^{-3} m \):\[ V_{max} = 3.0 \times 10^6 \times 1.5 \times 10^{-3} = 4500 \text{ V} \]Hence, the maximum voltage is \( 4500 \text{ V} \).
04

Calculate Energy Stored

The total energy \( U \) stored in the capacitor can be calculated using the formula:\[ U = \frac{1}{2} CV^2 \] Substitute \( C = 9 \times 10^{-11} F \) and \( V = 200 V \) into the equation:\[ U = \frac{1}{2} \times 9 \times 10^{-11} \times 200^2 \]\[ U = \frac{1}{2} \times 9 \times 10^{-11} \times 40000 = 1.8 \times 10^{-6} J \]Thus, the energy stored is \( 1.8 \times 10^{-6} J \).

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Key Concepts

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

Capacitance Formula
The capacitance formula is essential for understanding how capacitors work. Capacitance is defined as the ability of a capacitor to store charge. It can be calculated using the formula: \[ C = \frac{Q}{V} \] where \(C\) is the capacitance in farads (F), \(Q\) is the charge in coulombs (C), and \(V\) is the potential difference in volts (V) across the capacitor.

In this specific example, an air capacitor has a charge \(Q = 0.0180 \mu C\) or \(1.8 \times 10^{-8} C\), with a voltage \(V = 200 V\). By plugging these values into the formula, we find the capacitance \(C\) to be \(9.0 \times 10^{-11} F\).

This formula shows that capacitance is directly related to the amount of charge a capacitor can hold at a given voltage. This makes it a crucial concept for designing circuits that require precise energy management.
Parallel Plate Capacitors
Parallel plate capacitors are one of the simplest and most commonly used types of capacitors. They consist of two conductive plates separated by a small distance, with an insulating material called a dielectric in between.

The capacitance of a parallel plate capacitor can also be calculated using the formula:

\[ C = \frac{\varepsilon_0 A}{d} \] Here, \(\varepsilon_0\) represents the permittivity of free space, which is \(8.85 \times 10^{-12} \ F/m\), \(A\) is the area of one plate in square meters \(m^2\), and \(d\) is the distance between the plates in meters.

From our example, by rearranging the formula to find the area \(A\) and substituting the capacitance \(C = 9 \times 10^{-11} F\) and distance \(d = 1.5 \times 10^{-3} m\), we calculate the plate area to be approximately \(1.53 \times 10^{-2} m^2\).

Understanding the dimensions and separation of the plates helps in designing capacitors for specific applications, ensuring efficient energy storage and discharge.
Dielectric Breakdown
Dielectric breakdown is a critical factor to consider when working with capacitors. It occurs when the electric field strength in a dielectric exceeds its breakdown threshold, resulting in a loss of insulating properties and potentially causing damage.

For air, the breakdown electric field strength is approximately \(3.0 \times 10^6 \ V/m\). To find the maximum voltage \(V_{max}\) that can be applied to our capacitor without causing breakdown, we use:

\[ V_{max} = E_{break} \times d \] Substituting the breakdown field strength \(E_{break}\) and the plate distance \(d\), we find that the maximum safe voltage is \(4500 V\).

This value is essential for engineers and scientists to ensure capacitors are used safely and within their operational limits, preventing electrical failures in circuits.
Energy Storage in Capacitors
Capacitors are widely used for energy storage due to their ability to quickly charge and discharge. The energy \(U\) stored in a capacitor can be calculated using the equation:

\[ U = \frac{1}{2} CV^2 \] Where \(C\) is the capacitance and \(V\) is the voltage applied across the capacitor.

With a capacitance of \(9 \times 10^{-11} F\) and a voltage of \(200 V\), the energy stored in our example capacitor is \(1.8 \times 10^{-6} J\).

This calculation is essential in applications ranging from simple power supply filtering to complex energy systems where precise energy delivery is required. Capacitors provide a stable energy reserve that can be crucial for various electronic functions.

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Most popular questions from this chapter

24.38. Two parallel plates have equal and opposite charges. When the space between the plates is evacuated, the electric field is \(E=3.20 \times 10^{5} \mathrm{V} / \mathrm{m}\) . When the space is filled with dielectric, the electric field is \(E=2.50 \times 10^{5} \mathrm{V} / \mathrm{m}\) . (a) What is the charge density on each surface of the dielectric? (b) What is the dielectric constant?

24.28. A capacitor of capacitance \(C\) is charged to a potential difference \(V_{0}\) . The terminals of the charged capacitor are then connected to those of an uncharged capacitor of capacitance \(C / 2\) Compute (a) the original charge of the system; (b) the final potential difference across each capacitor; (e) the final energy of the system; (d) the decrease in energy when the capacitors are connected. (e) Where did the "lost" energy go?

24.48 . A parallel-plate capacitor has plates with area 0.0225 \(\mathrm{m}^{2}\) separated by 1.00 \(\mathrm{mm}\) of Tefion. (a) Calculate the charge on the plates when they are charged to a potential difference of 12.0 \(\mathrm{V}\) . (b) Use Gauss's law (Eq. 24.23 ) to calculate the electric field inside the Teflon. (c) Use Gauss's law to calculate the electric field if the voltage source is disconnected and the Teflon is removed.

24.40. A budding electronics hobbyist wants to make a simple 1.0 -nF capacitor for tuning her crystal radio, using two sheets of aluminum foil as plates, with a few shects of paper between them as a dielectric. The paper has a dielectric constant of 3.0, and the thickness of one sheet of it is 0.20 \(\mathrm{mm}\) . (a) If the sheets of paper measure \(22 \times 28 \mathrm{cm}\) and she cuts the aluminum foil to the same dimensions, how many sheets of paper should she use between her plates to get the proper capacitance? (b) Suppose for convenience she wants to use a single sheet of posterboard, with the same dielectric constant but a thickness of \(120 \mathrm{mm},\) instead of the paper. What area of aluminum foil will she need for her plates to get her 1.0 \(\mathrm{nF}\) of capacitance? (c) Suppose she goes hight-tech and finds a sheet of Teflon of the same thickness as the posterboard to use as a dielectric. Will she need a larger or smaller area of Tellon than of posterboard? Explain.

24.29. A parallel-plate vacuum capacitor with plate area \(A\) and separation \(x\) has charges \(+Q\) and \(-Q\) on its plates. The capacitor is disconnected from the source of charge, so the charge on each plate remains fixed. (a) What is the total energy stored in the capacitor? (b) The plates are pulled apart an additional distance \(d x\) . What is the change in the stored energy? (c) If \(F\) is the force with which the plates attract each other, then the change in the stored energy must equal the work \(d W=F d x\) done in pulling the plates apart. Find an expression for \(F\) (d) Explain why \(F\) is not equal to \(Q E\) , where \(E\) is the electric field between the plates.

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