Problem 20
Question
A uniform electric field of \(10 \mathrm{kV} / \mathrm{m}\) points vertically upward. How far apart are the equipotential planes that differ by \(100 \mathrm{~V} ?\)
Step-by-Step Solution
Verified Answer
The distance is 1 cm.
1Step 1: Understanding the Problem
We have a uniform electric field with a magnitude of \(10 \text{ kV/m}\) pointing upward. We need to find the distance between equipotential planes that have a potential difference of \(100\text{ V}\).
2Step 2: Key Formula for Distance in Electric Field
The relationship between electric potential difference \(\Delta V\), electric field \(E\), and distance \(d\) is given by the formula: \(\Delta V = E \times d\). We can rearrange this formula to solve for \(d\): \(d = \frac{\Delta V}{E}\).
3Step 3: Substituting Values
Substitute the given values into the formula: \(\Delta V = 100\text{ V} \) and \(E = 10 \times 10^3 \text{ V/m} \). So, \(d = \frac{100}{10 \times 10^3}\).
4Step 4: Calculate the Distance
By calculating the expression from the previous step, we find that \(d = \frac{100}{10000} = 0.01\) meters or \(1\) centimeter.
Key Concepts
Equipotential PlanesElectric Potential DifferenceDistance in Electric Fields
Equipotential Planes
In the context of electric fields, equipotential planes are imaginary surfaces where the electric potential is the same at every point. These planes are crucial because they simplify the study of electric fields, especially in uniform fields.
Equipotential planes are always perpendicular to the direction of the electric field. Therefore, if you have a uniform electric field pointing vertically upward, the equipotential planes will be horizontal. This perpendicularity ensures no work is required to move a charge along these planes, as the potential energy remains constant.
In practice, these planes can be visualized by imagining layers that never intersect each other. Think of them as flat sheets stacked parallel above one another, with each sheet representing a different potential level.
Equipotential planes are always perpendicular to the direction of the electric field. Therefore, if you have a uniform electric field pointing vertically upward, the equipotential planes will be horizontal. This perpendicularity ensures no work is required to move a charge along these planes, as the potential energy remains constant.
In practice, these planes can be visualized by imagining layers that never intersect each other. Think of them as flat sheets stacked parallel above one another, with each sheet representing a different potential level.
Electric Potential Difference
The electric potential difference, often referred to simply as voltage, is a measure of the work done to move a unit charge between two points in an electric field. It tells us how much potential energy has changed from one plane to another.
The formula for electric potential difference is
This equation helps determine
The formula for electric potential difference is
- \( \Delta V = E \times d \)
This equation helps determine
- how energy changes with distance in a field,
- and whether the field is capable of doing work on a charge.
Distance in Electric Fields
In a uniform electric field, the distance between equipotential planes is directly related to the electric potential difference and the strength of the electric field. The previously mentioned formula \( \Delta V = E \times d \) is rearranged to find distance as:
This means that as the electric field intensity increases, the distance between equipotential planes decreases for the same potential difference. Vice versa, for a specific field strength, greater potential differences indicate larger stretches between planes.
Understanding how to calculate and interpret these distances is essential in practical applications, like designing electronic circuits and analyzing field distributions.
- \( d = \frac{\Delta V}{E} \)
This means that as the electric field intensity increases, the distance between equipotential planes decreases for the same potential difference. Vice versa, for a specific field strength, greater potential differences indicate larger stretches between planes.
Understanding how to calculate and interpret these distances is essential in practical applications, like designing electronic circuits and analyzing field distributions.
Other exercises in this chapter
Problem 12
It takes +6.0 J of work to move two charges from a large distance apart to \(1.0 \mathrm{~cm}\) from one another. If the charges have the same magnitude, (a) ho
View solution Problem 13
\(\mathrm{A}+2.0-\mu \mathrm{C}\) charge is initially \(0.20 \mathrm{~m}\) from a fixed \(-5.0-\mu C\) charge and is then moved to a position \(0.50 \mathrm{~m}
View solution Problem 24
If the radius of the equipotential surface of a point charge is \(10.5 \mathrm{~m}\) and is at a potential of \(+2.20 \mathrm{kV}\) (compared to zero at infinit
View solution Problem 25
(a) The equipotential surfaces in the neighborhood of a positive point charge are spheres. Which sphere is associated with the higher electric potential: (1) th
View solution