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A small metal sphere, carrying a net charge of \(q_1 = -\)2.80 \(\mu\)C, is held in a stationary position by insulating supports. A second small metal sphere, with a net charge of \(q_2 = -\)7.80 \(\mu\)C and mass 1.50 g, is projected toward \(q_1\). When the two spheres are 0.800 m apart, \(q_2\), is moving toward \(q_1\) with speed 22.0 m\(/\)s (\(\textbf{Fig. E23.5}\)). Assume that the two spheres can be treated as point charges. You can ignore the force of gravity. (a) What is the speed of \(q_2\) when the spheres are 0.400 m apart? (b) How close does \(q_2\) get to \(q_1\)?

Short Answer

Expert verified
(a) 12.5 m/s, (b) 0.322 m.

Step by step solution

01

Understand the Problem

We have two charges, one stationary (\(q_1\)) and another moving towards it (\(q_2\)), both negative. We want to find the speed of \(q_2\) when the distance between them decreases and determine the point of closest approach by using conservation of energy.
02

Define Initial Energy Conditions

Initially, when the distance between \(q_1\) and \(q_2\) is 0.800 m, the kinetic energy \(KE_0\) of \(q_2\) is \( \frac{1}{2}mv^2 \) and its potential energy \(U_0\) is given by Coulomb's law: \[ U_0 = k\frac{q_1q_2}{r_0} \]where \(k = 8.99 \times 10^9 \, \text{N m}^2/\text{C}^2 \) is Coulomb's constant, \(r_0 = 0.800 \, \text{m}\), and \(v = 22.0 \, \text{m/s}\).
03

Calculate Initial Kinetic Energy

The initial kinetic energy \(KE_0\) of \(q_2\) when it is 0.800 m away is:\[ KE_0 = \frac{1}{2} \times 0.0015 \, \text{kg} \times (22.0 \, \text{m/s})^2 \]Execute the calculation:\[ KE_0 = \frac{1}{2} \times 0.0015 \times 484 = 0.362 \, \text{J} \]
04

Calculate Initial Potential Energy

Calculate the initial potential energy \(U_0\) of the system:\[ U_0 = 8.99 \times 10^9 \times \frac{(-2.80 \times 10^{-6})(-7.80 \times 10^{-6})}{0.800} \]Perform the calculation:\[ U_0 = 8.99 \times 10^9 \times \frac{21.84 \times 10^{-12}}{0.800} = 0.245 \, \text{J} \]
05

Apply Conservation of Energy at 0.400 m

The total mechanical energy initially \(E_0 = KE_0 + U_0 = 0.362 + 0.245 = 0.607 \, \text{J}\). When \(q_2\) is 0.400 m apart from \(q_1\), the potential energy \(U_1\) is:\[ U_1 = 8.99 \times 10^9 \times \frac{21.84 \times 10^{-12}}{0.400} = 0.490 \, \text{J} \]Using conservation of energy, solve for \(KE_1 = E_1 - U_1 = 0.607 - 0.490 = 0.117 \, \text{J}\).
06

Solve for Speed at 0.400 m

Given \(KE_1 = \frac{1}{2} mv_{0.400}^2 = 0.117 \, \text{J}\), solve for velocity \(v_{0.400}\):\[ \frac{1}{2} \times 0.0015 \times v_{0.400}^2 = 0.117 \rightarrow v_{0.400}^2 = \frac{0.117}{0.00075} = 156 \]Then:\[ v_{0.400} = \sqrt{156} = 12.5 \, \text{m/s} \]
07

Analyze the Closest Distance (Point of Turning)

At the closest point of approach, the speed of \(q_2\) is zero, so all kinetic energy is converted to potential energy. Thus, set the initial total energy equal to the potential energy at the turning point:\[ E_0 = U_f = k\frac{q_1q_2}{r_f} \]\(0.607 = 8.99 \times 10^9 \times \frac{21.84 \times 10^{-12}}{r_f}\) solving for \(r_f\):\[ r_f = \frac{8.99 \times 10^9 \times 21.84 \times 10^{-12}}{0.607} \approx 0.322 \, \text{m} \]
08

Answer Questions

(a) The speed of \(q_2\) when the spheres are 0.400 m apart is 12.5 m/s. (b) The closest approach to \(q_1\) is approximately 0.322 m.

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Key Concepts

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

Conservation of Energy
Conservation of Energy is a fundamental concept that states energy cannot be created or destroyed; it can only change from one form to another. In electrostatics, this principle is crucial to solving problems involving point charges.
When dealing with two charged objects, like the spheres in the exercise, both kinetic and potential energy are considered for each state's energy. The total energy of the system (kinetic plus potential) remains constant unless an external force acts. Initially, the energy is divided between the kinetic energy of the moving charge and the electrostatic potential energy due to their interactions.
To apply this concept:- Calculate the initial kinetic energy using the formula: \[ KE = \frac{1}{2}mv^2 \]- Determine the initial potential energy using Coulomb's law: \[ U = k\frac{q_1q_2}{r} \]- Ensure the sum of these energies at any two points is equal.This principle helps us find unknowns, such as the speed at different distances or the point of closest approach, by knowing that the total mechanical energy (kinetic and potential) doesn't change.
Point Charges
In electrostatics, charges are often simplified to point charges which have dimensions so small that their size doesn't affect the calculations of forces and fields around them. This idealization assists in applying mathematical formulas straightforwardly and understanding interactions at a simplistic level.
Point charges interact according to their position and charge magnitude, which determines the amount of electric force or potential energy involved. These charges can attract or repel, generating energies that influence the behavior of charged objects.
Examples of applying point charge assumptions in calculations include:- When finding the potential energy, use the formula considering them as point charges: \[ U = k \frac{q_1 q_2}{r} \]- Creations of electric fields are simplified to a point originating from a single location in space.Treating charges as point charges helps solve electrostatic problems more easily by focusing only on their separation distance and charge magnitudes.
Coulomb's Law
Coulomb's Law describes the electrostatic interaction between two point charges. By it, the magnitude of the force between any two charges is directly proportional to the product of their charge magnitudes and inversely proportional to the square of the distance that separates them.
The formula for Coulomb’s Law is: \[ F = k \frac{|q_1q_2|}{r^2} \]where:
  • F is the magnitude of the force between the charges.
  • k is Coulomb's constant ( 8.99 × 109 N m2/C2).
  • q_1 and q_2 are the amounts of the charges.
  • r is the separation distance between the charges.
Coulomb's Law is essential in calculations determining potential energy between charges. It explains why like charges repel and opposites attract, influencing the kinetic motion of charged particles, such as how they move towards or away from each other based on their interactions.

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Most popular questions from this chapter

(a) If a spherical raindrop of radius 0.650 mm carries a charge of \(-\)3.60 pC uniformly distributed over its volume, what is the potential at its surface? (Take the potential to be zero at an infinite distance from the raindrop.) (b) Two identical raindrops, each with radius and charge specified in part (a), collide and merge into one larger raindrop. What is the radius of this larger drop, and what is the potential at its surface, if its charge is uniformly distributed over its volume?

A thin insulating rod is bent into a semicircular arc of radius \(a\), and a total electric charge \(Q\) is distributed uniformly along the rod. Calculate the potential at the center of curvature of the arc if the potential is assumed to be zero at infinity.

A very long insulating cylinder of charge of radius 2.50 cm carries a uniform linear density of 15.0 nC\(/\)m. If you put one probe of a voltmeter at the surface, how far from the surface must the other probe be placed so that the voltmeter reads 175 V?

A solid conducting sphere has net positive charge and radius \(R =\) 0.400 m. At a point 1.20 m from the center of the sphere, the electric potential due to the charge on the sphere is 24.0 V. Assume that \(V = 0\) at an infinite distance from the sphere. What is the electric potential at the center of the sphere?

Two point charges of equal magnitude \(Q\) are held a distance \(d\) apart. Consider only points on the line passing through both charges. (a) If the two charges have the same sign, find the location of all points (if there are any) at which (i) the potential (relative to infinity) is zero (is the electric field zero at these points?), and (ii) the electric field is zero (is the potential zero at these points?). (b) Repeat part (a) for two point charges having opposite signs.

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