Problem 22
Question
At a certain distance from a point charge, the potential and electric-field magnitude due to that charge are 4.98 V and 16.2 V\(/\)m, respectively. (Take \(V = 0\) at infinity.) (a) What is the distance to the point charge? (b) What is the magnitude of the charge? (c) Is the electric field directed toward or away from the point charge?
Step-by-Step Solution
Verified Answer
(a) The distance is 0.307 m. (b) The magnitude of the charge is approximately \(1.7 \times 10^{-10}\) C. (c) The electric field is directed away from the charge.
1Step 1: Understanding the Relationships
Understand that the electric potential \( V \) and electric field \( E \) for a point charge \( Q \) at a distance \( r \) are given by \( V = \frac{kQ}{r} \) and \( E = \frac{kQ}{r^2} \) respectively, where \( k \) is Coulomb's constant (\( 8.99 \times 10^9 \, \text{N} \cdot \text{m}^2/\text{C}^2 \)). The goal is to find \( r \) and \( Q \).
2Step 2: Finding the Distance to the Point Charge
By dividing the formula for \( V \) by the formula for \( E \), we get: \( \frac{V}{E} = r \). Plug the known values into this equation: \( \frac{4.98}{16.2} = r \), yielding \( r = 0.307 \) m.
3Step 3: Calculating the Magnitude of the Charge
Using the value of \( r = 0.307 \) m and the formula for \( V \) (\( V = \frac{kQ}{r} \)), we solve for \( Q \). Rearrange to find \( Q = \frac{Vr}{k} \). Substituting the known values, \( Q = \frac{4.98 \times 0.307}{8.99 \times 10^9} \), resulting in \( Q \approx 1.7 \times 10^{-10} \) C.
4Step 4: Determining the Direction of the Electric Field
Since the electric field magnitude \( E \) and potential \( V \) are both positive, the point charge \( Q \) is positive. The electric field is directed away from positive charges.
Key Concepts
Electric PotentialElectric FieldCoulomb's Law
Electric Potential
Electric potential is a scalar quantity that is associated with the electric field a charge produces. It is the amount of work needed to move a unit positive charge from a reference point (typically at infinity) to a specific point in the space around a charge, without any acceleration. This is expressed as the potential energy per unit charge.
For a point charge, the electric potential at a distance \( r \) from the charge \( Q \) is given by the formula:
In the original problem, the potential \( V \) given is 4.98 V, suggesting the work done per unit charge to move it from infinity to the current position is 4.98 joules.
This scalar nature means that unlike vector quantities, potentials can be added algebraically without considering direction, making calculations straightforward.
Understanding electric potential is key to solving many electrostatics problems, especially those involving energy considerations.
For a point charge, the electric potential at a distance \( r \) from the charge \( Q \) is given by the formula:
- \( V = \frac{kQ}{r} \)
In the original problem, the potential \( V \) given is 4.98 V, suggesting the work done per unit charge to move it from infinity to the current position is 4.98 joules.
This scalar nature means that unlike vector quantities, potentials can be added algebraically without considering direction, making calculations straightforward.
Understanding electric potential is key to solving many electrostatics problems, especially those involving energy considerations.
Electric Field
The electric field is a vector field that represents the force experienced by a test charge at any point in space due to other charge distributions. It tells us the magnitude and direction of the force that would be felt by a unit positive charge placed at any given point.
For a point charge, the electric field \( E \) can be calculated using the equation:
It's vectorial nature makes the electric field more complex to deal with compared to scalar quantities like electric potential. It involves directional considerations. For example, the electric field direction is determined by the nature of the source charge; it points away from positive charges and towards negative ones.
Grasping the concept of electric fields aids in visualizing how charges influence their surroundings and helps solve problems related to forces and motion under electric influences.
For a point charge, the electric field \( E \) can be calculated using the equation:
- \( E = \frac{kQ}{r^2} \)
It's vectorial nature makes the electric field more complex to deal with compared to scalar quantities like electric potential. It involves directional considerations. For example, the electric field direction is determined by the nature of the source charge; it points away from positive charges and towards negative ones.
Grasping the concept of electric fields aids in visualizing how charges influence their surroundings and helps solve problems related to forces and motion under electric influences.
Coulomb's Law
Coulomb's law is the foundational principle that describes how charged particles interact with one another. It mathematically defines the electric force between two point charges.
The law is represented by the equation:
This concept is crucial for understanding electric interactions. It tells us:
The law is represented by the equation:
- \( F = \frac{k|Q_1 Q_2|}{r^2} \)
This concept is crucial for understanding electric interactions. It tells us:
- The force is inversely proportional to the square of the distance, meaning it decreases rapidly with distance.
- The force's magnitude is proportional to the product of the magnitudes of the charges involved.
- Opposite charges attract, so the force is negative, while like charges repel, resulting in a positive force.
Other exercises in this chapter
Problem 20
(a) An electron is to be accelerated from 3.00 \(\times 10^6\) m\(/\)s to 8.00 \(\times 10^6\) m\(/\)s. Through what potential difference must the electron pass
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A positive charge \(q\) is fixed at the point \(x = 0, y = 0\), and a negative charge \(-2_q\) is fixed at the point \(x = a, y = 0\). (a) Show the positions of
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A uniform electric field has magnitude \(E\) and is directed in the negative \(x\)-direction. The potential difference between point \(a\) (at \(x =\) 0.60 m) a
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For each of the following arrangements of two point charges, find all the points along the line passing through both charges for which the electric potential \(
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