/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 46 The same voltage is applied betw... [FREE SOLUTION] | 91Ó°ÊÓ

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The same voltage is applied between the plates of two different capacitors. When used with capacitor A, this voltage causes the capacitor to store \(11 \mu \mathrm{C}\) of charge and \(5.0 \times 10^{-5} \mathrm{J}\) of energy. When used with capacitor \(\mathrm{B}\) which has a capacitance of \(6.7 \mu \mathrm{F}\), this voltage causes the capacitor to store a charge that has a magnitude of \(q_{\mathrm{B}} .\) Determine \(q_{\mathrm{B}}\).

Short Answer

Expert verified
\(q_B = 69.3 \mu C\).

Step by step solution

01

Understanding the Problem

We have two capacitors, A and B, connected to the same voltage source. We need to find the charge stored in capacitor B, denoted as \(q_B\), given its capacitance and the fact that the voltage across both capacitors is equal.
02

Relate Voltage and Charge for Capacitor A

Let's use the relationship between energy \(E\), charge \(q\), and capacitance \(C\) for capacitor A. We have the formula for stored energy \(E = \frac{1}{2} C V^2\), where \(V\) is the voltage across the capacitor. We also know that \(q = C V\). Given: \(q_A = 11 \mu C\) and \(E_A = 5.0 \times 10^{-5} J\).
03

Calculate Capacitance of Capacitor A

Rearrange the energy formula to find capacitance: \(C_A = \frac{2E_A}{V^2}\). Substitute \(V = \frac{q_A}{C_A}\) into the energy equation: \(E_A = \frac{1}{2} C_A \left(\frac{q_A}{C_A}\right)^2\). Simplify to find \(C_A = \frac{q_A^2}{2E_A}\).
04

Substitute Values for Capacitor A

Substitute the known values into the formula: \(C_A = \frac{(11 \times 10^{-6} C)^2}{2 \times 5.0 \times 10^{-5} J}\). Calculate \(C_A\).
05

Calculate Voltage across Capacitors

With \(C_A\) calculated, find \(V_A\) using \(V_A = \frac{q_A}{C_A}\). Since \(V_A = V_B\), this gives us the voltage across capacitor B.
06

Find Charge on Capacitor B

Using the voltage \(V\) found and the capacitance of capacitor B, which is \(6.7 \mu F\), use \(q_B = C_B \times V_B\) to calculate \(q_B\).
07

Substitute Values to Calculate \(q_B\)

Substitute the value of \(C_B = 6.7 \times 10^{-6} F\) and the voltage \(V\) found previously into the equation \(q_B = C_B \times V\). Compute \(q_B\).
08

Conclusion

Verify that all steps have been followed correctly and check calculations to ensure that the final value of \(q_B\) aligns with the given energy conditions.

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Key Concepts

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

Capacitance
Capacitance is a fundamental property of capacitors. It defines a capacitor’s ability to store an electric charge. When you think of capacitance, imagine a container filling up with liquid. The bigger the container, the more it can hold. Capacitors work similarly but with electric charge. The unit of capacitance is the farad (F). However, due to the large size of one farad, practical capacitors often have values in microfarads (\( \mu F \)) or picofarads.
Capacitors are characterized by two main things:
  • Plate Size: Larger plates can store more charge.
  • Distance Between Plates: A smaller distance increases capacitance.
Capacitance is determined using the formula \( C = \frac{q}{V} \), where \( q \) is the charge stored, and \( V \) is the voltage applied. Understanding this relation helps clarify why capacitor B, with its given capacitance of \(6.7 \mu F\), stores a specific amount of charge when a certain voltage is applied. The higher the capacitance, for a given voltage, the more charge a capacitor can store. This is because a high capacitance allows more electric field lines to be stored between the capacitor plates.
Charge Storage
Charge storage in capacitors is an essential concept in electrostatics. Capacitors store energy as electric charge, ready to be discharged when needed, similar to a battery. The stored charge in a capacitor is directly proportional to the voltage applied across it. This phenomenon is described by the equation \( q = C \times V \), where \( q \) is the charge, \( C \) is the capacitance, and \( V \) is the voltage.
  • Higher voltage or higher capacitance will result in more charge being stored.
  • The amount of charge doesn't depend solely on the capacitance or voltage but on their product.
In this specific exercise, capacitor B stores a charge calculated as \(q_B = C_B \times V_B\). This charge storage capacity is why capacitors are so valuable in circuits, as they allow for the rapid storage and discharge of energy. Understanding how the capacitance and voltage influence charge storage can help predict the behavior of capacitor B in this scenario.
Energy in Capacitors
The energy stored in capacitors is one of their most useful properties. When a charge is stored in a capacitor, energy is also stored. This energy can be used to power devices momentarily when required. The relationship between energy stored in a capacitor, the charge, and the voltage is given by the equation: \( E = \frac{1}{2} C V^2 \).
  • Energy increases with greater charge and greater voltage.
  • The energy is a quadratic function of voltage, meaning that doubling the voltage quadruples the stored energy.
Capacitor A in this exercise stores an energy of \(5.0 \times 10^{-5}\, \mathrm{J}\) thanks to the charge \(11 \mu C\) and its capacitance. It demonstrates how changes in voltage affect energy storage. Calculating the energy helps engineers and scientists anticipate how much power a capacitor can deliver. For capacitor B, although we didn't directly calculate its energy, understanding its capacitance and the applied voltage helps assess the potential energy it can store.

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Most popular questions from this chapter

Two capacitors are identical, except that one is empty and the other is filled with a dielectric \((\kappa=4.50) .\) The empty capacitor is connected to a \(12.0-\mathrm{V}\) battery. What must be the potential difference across the plates of the capacitor filled with a dielectric so that it stores the same amount of electrical energy as the empty capacitor?

A charge of \(-3.00 \mu \mathrm{C}\) is fixed in place. From a horizontal distance of \(0.0450 \mathrm{m},\) a particle of \(\operatorname{mass} 7.20 \times 10^{-3} \mathrm{kg}\) and charge \(-8.00 \mu \mathrm{C}\) is fired with an initial speed of \(65.0 \mathrm{m} / \mathrm{s}\) directly toward the fixed charge. How far does the particle travel before its speed is zero?

What is the capacitance of a capacitor that stores \(4.3 \mu \mathrm{C}\) of charge on its plates when a voltage of \(1.5 \mathrm{V}\) is applied between them?

Two identical point charges \(\left(q=+7.20 \times 10^{-6} \mathrm{C}\right)\) are fixed at diagonally opposite corners of a square with sides of length \(0.480 \mathrm{m}\). A test charge \(\left(q_{0}=-2.40 \times 10^{-8} \mathrm{C}\right),\) with a mass of \(6.60 \times 10^{-8} \mathrm{kg},\) is released from rest at one of the empty corners of the square. Determine the speed of the test charge when it reaches the center of the square.

Charges of \(-q\) and \(+2 q\) are fixed in place, with a distance of \(2.00 \mathrm{m}\) between them. A dashed line is drawn through the negative charge, perpendicular to the line between the charges. On the dashed line, at a distance \(L\) from the negative charge, there is at least one spot where the total potential is zero. Find \(L\).

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