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An electron is released from rest at the negative plate of a parallel plate capacitor and accelerates to the positive plate (see the drawing). The plates are separated by a distance of \(1.2 \mathrm{cm},\) and the electric field within the capacitor has a magnitude of \(2.1 \times 10^{6} \mathrm{V} / \mathrm{m} .\) What is the kinetic energy of the electron just as it reaches the positive plate?

Short Answer

Expert verified
The kinetic energy of the electron is approximately \(4.032 \times 10^{-15} \text{ J}\).

Step by step solution

01

Understanding the Motion and Energy Conversion

The electron is initially at rest at the negative plate, so its initial kinetic energy is 0. When it reaches the positive plate, all the work done by the electric field on the electron has been converted into kinetic energy.
02

Determine the Potential Difference (Voltage)

The potential difference between two plates of a capacitor is given by the product of the electric field (E) and the separation distance (d) between the plates.\[V = E \times d = 2.1 \times 10^{6} \text{ V/m} \times 0.012 \text{ m}\]Calculating this, we get:\[V = 2.52 \times 10^{4} \text{ V}\]
03

Calculate the Kinetic Energy from the Potential Difference

The work done on the electron, which turns into kinetic energy (K.E.), is equal to the charge of the electron (e) times the potential difference (V) it travels through:\[K.E. = e \times V\]where the charge of the electron is e = 1.6 \times 10^{-19} \text{ C}. Substituting the values, we have:\[K.E. = 1.6 \times 10^{-19} \text{ C} \times 2.52 \times 10^{4} \text{ V}\]Calculating this gives:\[K.E. = 4.032 \times 10^{-15} \text{ J}\]
04

Conclude with Kinetic Energy Value

The kinetic energy of the electron just as it reaches the positive plate is determined by its acceleration due to the electric field across the capacitor plates, resulting in the value we calculated.

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Key Concepts

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

Electric Field
The concept of an electric field is crucial in understanding how charges interact over distances. An electric field is a region around a charged object where other charges feel a force. This invisible field is responsible for the acceleration of charges, such as electrons, within the field.

In our exercise, the electric field within the capacitor is uniform and has a magnitude of \(2.1 \times 10^6 \text{ V/m} \). This strong field exerts a force on the electron, pushing it across the capacitor from the negative to the positive plate. The magnitude indicates how strong the force exerted on a charge would be per unit charge.

Key points about the electric field within a parallel plate capacitor include:
  • The field is uniform, meaning it has the same magnitude and direction at every point between the plates.
  • It points from the positive to the negative plate inside a capacitor.
  • The strength of the field depends on the potential difference and the separation between the plates.
Potential Difference
Potential difference, also known as voltage, is a measure of the work needed to move a charge from one point to another within an electric field. It is the energy difference per charge between two positions. Thus, a high potential difference means more work can be done on the charge.

For our parallel plate capacitor, the potential difference is calculated by the formula: \[ V = E \times d \] where \( E \) is the electric field strength and \( d \) is the separation between the plates. Plugging in the values, we find \[ V = 2.1 \times 10^6 \, \text{V/m} \times 0.012 \, \text{m} = 2.52 \times 10^4 \, \text{V} \] This calculation shows the potential gain of an electron moving through the field.

Some important aspects of potential difference include:
  • It’s a scalar quantity, meaning it has size but no direction.
  • It represents the ability to do work on a charge.
  • Affects the speed at which charges move between two points.
Work-Energy Principle
The work-energy principle cleverly connects the concepts of work and energy. It states that the work done on an object is equal to the change in kinetic energy of that object.

In this exercise, an electron initially at rest gains kinetic energy as it moves across the capacitor due to the work done by the electric field. We use the potential difference (voltage) to calculate the work done on the charge, using the electron's charge \( e = 1.6 \times 10^{-19} \, \text{C} \). This work becomes the kinetic energy of the electron: \[ \text{K.E.} = e \times V = 1.6 \times 10^{-19} \, \text{C} \times 2.52 \times 10^4 \, \text{V} = 4.032 \times 10^{-15} \, \text{J} \]
Key points about the work-energy principle include:
  • Work leads to a change in energy states, typically converting potential energy to kinetic energy.
  • Kinetic energy depends on the velocity gained due to the work done.
  • Ensures energy conservation by transforming energy from one form to another.

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Most popular questions from this chapter

A charge of \(+125 \mu \mathrm{C}\) is fixed at the center of a square that is \(0.64 \mathrm{m}\) on a side. How much work is done by the electric force as a charge of \(+7.0 \mu \mathrm{C}\) is moved from one corner of the square to any other empty corner? Explain.

Two point charges, \(+3.40 \mu \mathrm{C}\) and \(-6.10 \mu \mathrm{C},\) are separated by \(1.20 \mathrm{m}\) What is the electric potential midway between them?

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 \(L\).

Equipotential surface \(A\) has a potential of \(5650 \mathrm{V},\) while equipotential surface \(B\) has a potential of 7850 V. A particle has a mass of \(5.00 \times\) \(10^{-2} \mathrm{kg}\) and a charge of \(+4.00 \times 10^{-5} \mathrm{C} .\) The particle has a speed of \(2.00 \mathrm{m} / \mathrm{s}\) on surface \(A\). A nonconservative outside force is applied to the particle, and it moves to surface \(B\), arriving there with a speed of \(3.00 \mathrm{m} / \mathrm{s}\). How much work is done by the outside force in moving the particle from \(A\) to \(B ?\)

'I'he membrane that surrounds a certain type of living cell has a surface area of \(5.0 \times 10^{-9} \mathrm{m}^{2}\) and a thickness of \(1.0 \times 10^{-8} \mathrm{m} .\) Assume that the membrane behaves like a parallel plate capacitor and has a dielectric constant of \(5.0 .\) (a) The potential on the outer surface of the membrane is \(+60.0 \mathrm{mV}\) greater than that on the inside surface. How much charge resides on the outer surface? (b) If the charge in part (a) is due to positive ions (charge \(+e\) ), how many such ions are present on the outer surface?

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