Problem 10
Question
Four electrons are located at the corners of a square 10.0 nm on a side, with an alpha particle at its midpoint. How much work is needed to move the alpha particle to the midpoint of one of the sides of the square?
Step-by-Step Solution
Verified Answer
Work needed is approximately \( 1.03 \times 10^{-18} \, \text{J} \).
1Step 1: Calculate Initial Potential Energy
The initial potential energy of the alpha particle at the center of the square is due to its interaction with the four electrons. The potential energy between the alpha particle and one electron is given by \[ U = \frac{k \cdot q_1 \cdot q_2}{r} \] where \( k = 8.99 \times 10^9 \, \text{Nm}^2/\text{C}^2 \) is Coulomb's constant, \( q_1 = +2e \) is the charge of the alpha particle, \( q_2 = -e \) is the charge of an electron, and \( r = \frac{\sqrt{2}a}{2} = 5\sqrt{2} \times 10^{-9} \, \text{m} \) is the distance from the alpha particle to an electron. Calculate \( U \) for each electron and sum the contributions.
2Step 2: Calculate Potential Energy at New Position
When the alpha particle is moved to the midpoint of one of the sides of the square, its distance from different electrons changes. Calculate the new distances: two electrons at distance \( a/2 = 5.0 \times 10^{-9} \, \text{m} \), one electron directly opposite the midpoint at distance \( a = 10.0 \times 10^{-9} \, \text{m} \), and one electron at distance \( \sqrt{5}a/2 = 5\sqrt{5} \times 10^{-9} \, \text{m} \). Use the potential energy formula to calculate the potential energy contribution from each electron, and sum these contributions.
3Step 3: Calculate Work Done
Work done on the system is the difference in potential energy between the final and initial positions of the alpha particle. Calculate it using:\[ W = U_{final} - U_{initial} \] Substitute the values of final and initial potential energies calculated in steps 1 and 2.
Key Concepts
Coulomb's LawWork-Energy PrincipleCharge InteractionsAlpha Particles
Coulomb's Law
Coulomb's law is a fundamental principle in electrostatics that helps us understand the forces and energy between charged particles. It describes how the electrostatic force between two charged objects is proportional to the product of their charges and inversely proportional to the square of the distance between them. This law is mathematically expressed as:
Using this law, you understood how to calculate the potential energy between the alpha particle and each of the electrons in the problem. Instead of focusing on the force directly, the exercise makes use of this law to determine the energy states, comparing them to find the work done by moving the alpha particle.
- \( F = \frac{k \cdot q_1 \cdot q_2}{r^2} \)
Using this law, you understood how to calculate the potential energy between the alpha particle and each of the electrons in the problem. Instead of focusing on the force directly, the exercise makes use of this law to determine the energy states, comparing them to find the work done by moving the alpha particle.
Work-Energy Principle
The work-energy principle is a key concept that connects the work done on an object to its energy. In electrostatics, the work done on a charged particle results in changes in its electrostatic potential energy.
The principle states:
By calculating the initial potential energy at the center of the square and the potential energy at a new position on the side, the change in energy gives us the work done moving the particle.
The principle states:
- The work done on an object is equal to the change in its energy.
- In our exercise, this translates to: \( W = U_{final} - U_{initial} \).
By calculating the initial potential energy at the center of the square and the potential energy at a new position on the side, the change in energy gives us the work done moving the particle.
Charge Interactions
Charge interactions are central to understanding why particles behave the way they do in an electric field. Like charges repel each other, while opposite charges attract. This fundamental behavior allows us to predict and calculate behavior in systems like the one in the exercise.
Charge interactions provide insight into why the alpha particle needs work to be moved to specific positions, as this involves altering the distances over which these attractive forces act.
- Electrons, having a negative charge, interact attractively with the positively charged alpha particle.
- The potential energy calculations made in the exercise depend heavily on these interactions.
Charge interactions provide insight into why the alpha particle needs work to be moved to specific positions, as this involves altering the distances over which these attractive forces act.
Alpha Particles
Alpha particles are a type of charged particle consisting of 2 protons and 2 neutrons. They are positively charged due to the protons, making them interact with other charged entities.
Since the alpha particle is positively charged, it is attracted to negatively charged electrons. This interaction defines the potential energy landscape we analyze.
In scenarios involving alpha particles, it is also significant to note their mass is relatively large compared to an electron, affecting how they move under electric forces. However, their charge is what primarily dictates their interaction in electrostatic situations like the one we've explored.
- In this exercise, the alpha particle had a charge of \(+2e\), where \(e\) is the elementary charge.
Since the alpha particle is positively charged, it is attracted to negatively charged electrons. This interaction defines the potential energy landscape we analyze.
In scenarios involving alpha particles, it is also significant to note their mass is relatively large compared to an electron, affecting how they move under electric forces. However, their charge is what primarily dictates their interaction in electrostatic situations like the one we've explored.
Other exercises in this chapter
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