Chapter 23: Problem 35
A very small sphere with positive charge \(q = +\)48.00 \(\mu\)C is released from rest at a point 1.50 cm from a very long line of uniform linear charge density \(\lambda = +\)3.00 \(\mu\)C\(/\)m. What is the kinetic energy of the sphere when it is 4.50 cm from the line of charge if the only force on it is the force exerted by the line of charge?
Short Answer
Step by step solution
Understand the Physical Scenario
Identify the Change in Distance
Calculate Initial and Final Electric Potential at Each Distance
Calculate the Potential Difference
Determine the Change in Electric Potential Energy
Use Conservation of Energy to Find Kinetic Energy
Final Calculation and Result
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Electric Potential
\[V = \frac{2k_e \lambda}{r}\]where:
- \( V \) is the electric potential,
- \( k_e \) is Coulomb's constant \( 8.99 \times 10^9 \, \text{N} \, \text{m}^2 \text{C}^{-2} \),
- \( \lambda \) is the linear charge density,
- \( r \) is the distance from the line.
Kinetic Energy
\[K = \frac{1}{2}mv^2\]However, in electrostatic problems without explicit mass and velocity information, we use changes in potential energy to find kinetic energy.This is due to conservation of energy which tells us:
\[\Delta U = -\Delta K\]If the initial kinetic energy is zero (as it starts from rest), the final kinetic energy \( K_f \) is equal to the change in electric potential energy \( \Delta U \).In short, the amount by which the electric potential energy decreases will entirely convert to kinetic energy for the moving charge, allowing us to calculate the speed or kinetic effects at different points in the field.
Linear Charge Density
\[\lambda = \frac{Q}{L}\]where:
- \( \lambda \) is the linear charge density,
- \( Q \) is the total charge,
- \( L \) is the length over which the charge is distributed.
Potential Energy
\[U = qV\]where:
- \( U \) is the electric potential energy,
- \( q \) is the charge of the object,
- \( V \) is the electric potential at that point.