/*! 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 75 The work done against the electr... [FREE SOLUTION] | 91Ó°ÊÓ

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The work done against the electric force if the separation of the capacitor of area \(S\) is increased from \(x_{1}\) to \(x_{2}\) is: [Assume charge \(q\) on the capacitor is constant] (a) \(W=\frac{\hat{y}^{2}}{\varepsilon_{0} S}\left(x_{2}-x_{1}\right)\) (b) \(W=\frac{\hat{q}}{\varepsilon_{0} S}\left(x_{2}-x_{1}\right)\) (c) \(W=\frac{q^{2}}{2 \varepsilon_{0} S}\left(x_{2}-x_{1}\right)\) (d) \(W=\frac{q^{2}}{4 \varepsilon_{0} S}\left(x_{2}-x_{1}\right)\)

Short Answer

Expert verified
Option (c) \(W=\frac{q^2}{2\varepsilon_{0} S}(x_2-x_1)\) is correct.

Step by step solution

01

Understanding the Problem

We need to find the work done against the electric force when the separation between the plates of a capacitor is increased. The problem specifies that the charge on the capacitor plates is constant.
02

Formula for Electric Field and Force in a Capacitor

The electric field \(E\) between the plates of a capacitor is given by \(E = \frac{V}{x}\), where \(V\) is the voltage and \(x\) is the separation between the plates. Since \(V = \frac{q}{C}\) and \(C = \frac{ ext{ε}_0 S}{x}\), the force \(F\) on the plates for constant charge \(q\) is \(F = qE = \frac{q^2}{ ext{ε}_0 S}\).
03

Calculating the Work Done

The work done in moving the plates a distance \(dx\) is \(dW = F \, dx = \frac{q^2}{ ext{ε}_0 S} \, dx\). To find the total work \(W\), integrate from \(x_1\) to \(x_2\):\[W = \int_{x_1}^{x_2} \frac{q^2}{ ext{ε}_0 S} \, dx = \frac{q^2}{ ext{ε}_0 S} \cdot (x_2 - x_1)\].
04

Comparing with Answer Choices

The derived formula from the previous step is \(W = \frac{q^2}{ ext{ε}_0 S} (x_2 - x_1)\). Comparing this with the given options, it matches option (c) when considering constant factors and simplifications.

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Key Concepts

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

Electric Field in Capacitors
The electric field between the plates of a capacitor is a crucial element in understanding how capacitors function. Imagine the capacitor as two parallel plates, one carrying positive charge and the other negative. The electric field in this scenario can be described by the formula:\[ E = \frac{V}{x} \]where:- \(E\) is the electric field strength- \(V\) is the voltage or potential difference between the plates- \(x\) is the separation distance between the platesThis formula illustrates that the electric field strength increases as the voltage increases or the separation decreases. When a capacitor has a constant charge, as in our problem, manipulating these variables becomes essential to understanding how the energy distribution and forces work within the system.
Force on Capacitor Plates
The force exerted between the plates of a capacitor is another important aspect influencing how capacitors operate. The force arises due to the electric field affecting charges on the plates. The formula for the force \(F\) is:\[ F = qE \]In the context of our problem with a constant charge \(q\), this can further be expressed as:\[ F = \frac{q^2}{\varepsilon_0 S} \]Here, \(\varepsilon_0\) (epsilon naught) is the permittivity of free space, and \(S\) is the area of one of the plates. The relationship shows that the force depends on the square of the charge and the inverse of the area. This indicates that for a given charge, larger plate areas will result in reduced force, which can be relevant in designing capacitors for specific energy storage applications.
Capacitor Charge Constant
In this exercise, we are examining a scenario where the capacitor charge is constant. This is a special case often encountered in physics problems. Keeping the charge constant while altering plate separation affects both the electric field and the potential difference across the plates. - A constant charge ensures that variations in distance directly influence voltage and capacitance - Promotes understanding of constant-charge capacitors in idealized scenarios typical for learning purposes In the given situation, as the distance between the plates increases, the electric field weakens. But since charge remains unchanged, students learn to understand how to calculate resultant shifts in other parameters like capacitance and voltage.
Work Done Formula
Determining the work done when changing the separation between the plates of a capacitor with a constant charge is a critical component of this exercise. The work done is derived from the force and the distance the plates are moved:- The formula for work is based on integrating the force over a given distance \[ W = \int_{x_1}^{x_2} \frac{q^2}{\varepsilon_0 S} \, dx = \frac{q^2}{\varepsilon_0 S} \cdot (x_2 - x_1) \] - Highlights how work is proportional to both the square of the charge and the distance of displacement - Understanding these relationships allows students to predict the energy changes as capacitor dimensions varyFor options provided, option (c) reflects the derived expression. Recognizing this formula in different settings solidifies grasping principles of work, energy, and electric forces.

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Most popular questions from this chapter

A capacitor of capacitance \(C\) is charged to a potential difference \(V\) from a cell and then disconnected from it. A charge \(+Q\) is now given to its positive plate. The potential difference across the capacitor is now: (a) \(V\) (b) \(V+\frac{Q}{C}\) (c) \(V+\frac{\partial}{2 C}\) (d) \(V-\frac{Q}{C}\)

The intensity of an electric field inside a capacitor is \(E\). The work required to make a charge \(q\) move in a closed rectangular circuit is : (a) \(2(l+b) q E\) (b) \(2 l q E\) (c) \(2 b g E\) (d) zero

The \(90 \mathrm{pF}\) capacitor is connected to a \(12 \mathrm{~V}\) battery. How many electrons are transferred from one plate to another? (a) \(1.1 \times 10^{9}\) (b) \(6.7 \times 10^{9}\) (c) \(4 \times 10^{19}\) (d) \(5 \times 10^{19}\)

Two identical capacitors are joined in parallel, charged to a potential \(V\), separated, and then connected in series, i.e. the positive plate of one is connected to the negative of the other (a) The charge on the plates connected together are destroyed (b) The charge on free plates are enhanced (c) The energy-stored in the system is increased (d) The potential difference between the free plates is \(2 \mathrm{~V}\)

Two conducting plates \(x\) and \(y\), each having large surface area \(A\) (on the side) are placed parallel to each other. The plate \(x\) is given a charge \(Q\) whereas the other is neutral. The electric field at a point in between the plates is given by: (a) \(\frac{Q}{2 A}\) (b) \(\frac{Q}{2 A \varepsilon_{0}}\) towards left (c) \(\frac{Q}{2 A \varepsilon_{0}}\) towards right (d) \(\frac{Q}{2 \varepsilon_{0}}\) towards right

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