A Particle Has A Charge Of Q = 2e, Where E Is The Charge On An Electron. (a) Determine The Electric Potential

A Particle Has A Charge Of Q = 2e, Where E Is The Charge On An Electron. (a) Determine The Electric Potential

Understanding electric potential and charge interactions is fundamental in physics, especially in electrostatics. When dealing with particles carrying electric charge, calculating the electric potential they produce is crucial for analyzing various phenomena, from atomic interactions to large-scale electromagnetic systems. In this article, we focus on a specific scenario: a particle with a charge \( Q = 2e \), where \( e \) is the elementary charge (the charge of a single electron). Our goal is to determine the electric potential created by this particle under given conditions.

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Fundamentals of Electric Charge and Electric Potential

Before delving into the specific problem, it’s essential to understand some basic concepts.

What Is Electric Charge?

Electric charge is a property of matter that causes it to experience a force when placed in an electric field. The two types of electric charges are positive and negative. The elementary charge, denoted by \( e \), is approximately:
  • \( e = 1.602 \times 10^{-19} \) coulombs (C)
A particle with charge \( Q = 2e \) thus has a positive charge twice that of an electron.

What Is Electric Potential?

Electric potential, often simply called potential, is the electric potential energy per unit charge at a point in space due to electric charges. It is a scalar quantity, measured in volts (V), where:
  • 1 volt = 1 joule/coulomb (J/C)
Physically, it represents the work done in bringing a unit positive charge from infinity to that point without acceleration.

Electric Potential Due to a Point Charge

The electric potential \( V \) at a distance \( r \) from a point charge \( Q \) is given by Coulomb's law:

\[
V = \frac{1}{4\pi \varepsilon_0} \times \frac{Q}{r}
\]

where:


  • \( \varepsilon_0 \) is the vacuum permittivity, approximately \( 8.854 \times 10^{-12} \, \text{F/m} \)

  • \( Q \) is the charge in coulombs

  • \( r \) is the distance from the charge in meters


This formula assumes the point charge is isolated in free space, and the potential is measured relative to a point at infinity where the potential is zero.

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Given Data and Problem Statement

The problem specifies:


  • The particle's charge: \( Q = 2e \)

  • \( e \): elementary charge \( \approx 1.602 \times 10^{-19} \, \text{C} \)


Our task:

  • To determine the electric potential \( V \) at a specific point or distance, based on the information provided.


Note: Since the problem statement does not specify the distance \( r \), for comprehensive understanding, we will analyze the potential at an arbitrary distance \( r \) from the particle, and later, if needed, evaluate for specific distances.

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Step-by-Step Calculation of Electric Potential

1. Expressing the Charge \( Q \)

Since \( Q = 2e \):

\[
Q = 2 \times 1.602 \times 10^{-19} \, \text{C} = 3.204 \times 10^{-19} \, \text{C}
\]

2. Applying the Electric Potential Formula

Using Coulomb's law:

\[
V(r) = \frac{1}{4\pi \varepsilon_0} \times \frac{Q}{r}
\]

The constant \( \frac{1}{4\pi \varepsilon_0} \) is known as Coulomb's constant \( k \):

\[
k = 8.9875 \times 10^9 \, \text{Nm}^2/\text{C}^2
\]

Thus,

\[
V(r) = k \times \frac{Q}{r}
\]

Substituting the known values:

\[
V(r) = (8.9875 \times 10^9) \times \frac{3.204 \times 10^{-19}}{r}
\]

\[
V(r) = \frac{(8.9875 \times 10^9) \times 3.204 \times 10^{-19}}{r}
\]

Calculating numerator:

\[
8.9875 \times 10^9 \times 3.204 \times 10^{-19} \approx 2.880 \times 10^{-9}
\]

Therefore,

\[
V(r) = \frac{2.880 \times 10^{-9}}{r}
\]

where \( r \) is in meters, and \( V(r) \) will be in volts.

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Understanding the Significance of the Electric Potential

The potential \( V(r) \) reflects how the particle's charge influences the space around it. Key points include:


  • Potential at different distances: As \( r \) increases, the potential decreases proportionally, approaching zero at infinity.

  • Sign of potential: Since \( Q \) is positive (\( 2e \)), the potential is positive at all points, indicating a repulsive effect on other positive charges.


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Applications and Examples

To contextualize the calculation, here are some typical scenarios:

Example 1: Potential at 1 nm from the particle

Given \( r = 1\, \text{nm} = 1 \times 10^{-9} \, \text{m} \):

\[
V(1\, \text{nm}) = \frac{2.880 \times 10^{-9}}{1 \times 10^{-9}} = 2.880\, \text{V}
\]

This implies that at 1 nanometer from the particle, the electric potential is approximately 2.88 volts.

Example 2: Potential at 1 μm from the particle

Given \( r = 1\, \mu \text{m} = 1 \times 10^{-6} \, \text{m} \):

\[
V(1\, \mu \text{m}) = \frac{2.880 \times 10^{-9}}{1 \times 10^{-6}} = 2.88 \times 10^{-3} = 0.00288\, \text{V}
\]

The potential drops significantly with increasing distance.

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Considerations and Limitations

While the calculations above are straightforward for point charges in free space, several factors can influence real-world scenarios:


  • Medium effects: The presence of materials other than vacuum, such as dielectric substances, alters the permittivity and thus the potential.

  • Charge distribution: If the charge is not concentrated at a point but spread out, the potential calculation becomes more complex.

  • Boundary conditions: Near conductive surfaces or in systems with specific boundary conditions, potential calculations need to incorporate additional factors.


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Summary and Conclusion

In this comprehensive analysis, we have:


  • Clarified the concept of electric potential and its relation to point charges.

  • Calculated the electric potential generated by a particle with charge \( Q = 2e \) at an arbitrary distance \( r \).

  • Demonstrated how the potential diminishes with increasing distance.

  • Provided practical examples to illustrate the potential at nanoscale and microscale distances.


Final formula:

\[
V(r) = \frac{2.880 \times 10^{-9}}{r} \quad \text{(volts, with \( r \) in meters)}
\]

This fundamental calculation forms the basis for more complex electrostatic problems involving multiple charges, distribution of charge, and potential energy considerations in physics and engineering.

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Additional Resources for Further Study

  • Textbook: Introduction to Electrodynamics by David J. Griffiths
  • Online simulations: Coulomb’s Law and Electric Potential calculators
  • Educational videos: Electrostatics and Electric Potential explanations on platforms like Khan Academy
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Remember: Precise calculation of electric potential is essential for designing electronic devices, understanding atomic interactions, and exploring electromagnetic phenomena across various scientific fields.

Frequently Asked Questions

What is the value of the charge Q in terms of the elementary charge e?
The charge Q is given as Q = 2e, meaning it is twice the elementary charge e.
How is the electric potential V related to the charge Q and the electric potential due to a single electron?
The electric potential V at a point due to a charge Q is given by V = (k Q) / r, where k is Coulomb's constant and r is the distance from the charge to the point of interest.
How do you calculate the electric potential for a particle with charge Q = 2e?
To calculate the electric potential, multiply Coulomb's constant k by the charge Q = 2e, then divide by the distance r from the charge to the point where potential is measured: V = (k 2e) / r.
What is Coulomb's constant and its approximate value?
Coulomb's constant k is approximately 8.99 x 10^9 N·m²/C², and it relates electric force and charge.
If the distance r from the charge to the point of measurement is 1 meter, what is the electric potential for Q = 2e?
Using V = (k Q) / r with Q = 2e (~3.2 x 10^-19 C), r = 1 m, V ≈ (8.99 x 10^9 N·m²/C²) (3.2 x 10^-19 C) / 1 m ≈ 2.88 volts.
Why is understanding the electric potential important in analyzing charged particles like Q = 2e?
Electric potential helps determine the energy per unit charge at a point in the electric field, which is essential for understanding the behavior of charged particles, their interactions, and energy exchanges in electrostatic systems.