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Why do electric field lines never cross?

Short Answer

Expert verified
Answer: Electric field lines never cross because a single electric field line represents the unique direction of the electric force experienced by a positive test charge at any point in space. If they were to cross, it would imply that a test charge at the intersection could experience multiple force directions, which is contradictory. The principle of superposition ensures that the combined effect of multiple electric fields is represented by a single electric field line, preserving the uniqueness of the direction for a given point.

Step by step solution

01

Understand the concept of electric field lines

Electric field lines are imaginary lines that indicate the direction of the electric force experienced by a positive test charge placed in the electric field. The density of these lines at any region indicates the strength of the electric field at that point. A more concentrated region of lines indicates a stronger electric field, and a less concentrated region indicates a weaker field.
02

Consider the field lines at a point where they cross

If electric field lines were to cross, it would mean that at the point where they cross, there are two different directions of the electric force experienced by a positive test charge. This would be contradictory, as a charge can only experience a single force direction at any given point.
03

Recall the principle of superposition

The principle of superposition states that the net electric field at a point due to multiple sources is the vector sum of the individual electric fields created by each source. In other words, the electric field at a point is the result of the combination of the electric fields created by all charges present in the system.
04

Apply the principle of superposition to electric field lines

According to the principle of superposition, the electric field at a point due to different charges is not represented by separate lines but by a single line that represents the vector sum of all individual fields. The electric field at any point in space is unique and has a specific direction. So even if multiple sources contribute to the electric field at that point, there can only be one electric field line at that point.
05

Conclusion

Electric field lines never cross because a single electric field line represents the unique direction of the electric force experienced by a positive test charge at any point in space. If they were to cross, it would imply that a test charge at the intersection could experience multiple force directions, which is contradictory. The principle of superposition ensures that the combined effect of multiple electric fields is represented by a single electric field line, preserving the uniqueness of the direction for a given point.

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Key Concepts

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

Electric Force
Understanding the concept of electric force is fundamental in physics. It's the force between charged particles. When a positive test charge is placed in an electric field, it experiences an electric force that pushes or pulls it in a specific direction. This force is central to the behavior of electric charges and fields.

Imagine you have a single charged particle. It creates an electric field around it, and the strength of this field can be visualized through electric field lines. These lines radiate outward from the positive charge and indicate the direction that another positive charge would be pushed if placed within the field. These field lines help us visualize how charges interact with each other without physically observing the particles themselves.
Principle of Superposition
The principle of superposition plays a vital role in understanding complex electric field scenarios. It posits that the total electric field created by multiple charges is simply the vector sum of the individual fields produced by each charge.

For instance, if you have two charges in close vicinity, each creates its own electric field. To find the total field at any point, you add the vector fields produced by both charges. By considering each electric field's magnitude and direction, you can determine the resultant field's exact characteristics. This concept is critical because it allows us to analyze and predict the behavior of electric fields in the presence of multiple charges simply and effectively.
Vector Sum of Electric Fields
The idea of the vector sum of electric fields is integral when multiple sources influence the electric field at a point. To find the total field, we must consider not only the magnitude of each individual field but also its direction, because the electric field is a vector quantity.

When combining vector fields, we use vector addition. For two electric fields, \( \vec{E_1} \) and \( \vec{E_2} \) with different directions, their vector sum, \( \vec{E_{total}} \) is found by placing the tail of \( \vec{E_2} \) at the head of \( \vec{E_1} \) and drawing a vector from the tail of \( \vec{E_1} \) to the head of \( \vec{E_2} \) . This resultant vector represents the combined effect of all electric fields at a specific point.
Unique Direction of Electric Field
A key characteristic of electric fields is that they have a unique direction at any point in space. This means that for any given location, a positive test charge will only be pushed or pulled in one specific direction by the electric field.

Due to this uniqueness, electric field lines are drawn so that they never cross. If they did, it would imply the existence of two different directions at that point, which contradicts the single force direction a charge can experience. This unique direction is a critical concept when visualizing electric field patterns and aids in grasping the nature of electric forces in space.

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Most popular questions from this chapter

Which of the following statements is (are) true? a) There will be no change in the charge on the inner surface of a hollow conducting sphere if additional charge is placed on the outer surface. b) There will be some change in the charge on the inner surface of a hollow conducting sphere if additional charge is placed on the outer surface. c) There will be no change in the charge on the inner surface of a hollow conducting sphere if additional charge is placed at the center of the sphere. d) There will be some change in the charge on the inner surface of a hollow conducting sphere if additional charge is placed at the center of the sphere.

An infinitely long, solid cylinder of radius \(R=9.00 \mathrm{~cm},\) with a uniform charge per unit of volume of \(\rho=6.40 \cdot 10^{-8} \mathrm{C} / \mathrm{m}^{3},\) is centered about the \(y\) -axis. Find the magnitude of the electric field at a radius \(r=4.00 \mathrm{~cm}\) from the center of this cylinder.

A thin, hollow, metal cylinder of radius \(R\) has a surface charge distribution \(\sigma\). A long, thin wire with a linear charge density \(\lambda / 2\) runs through the center of the cylinder. Find an expression for the electric field and determine the direction of the field at each of the following locations: a) \(r \leq R\) b) \(r \geq R\)

Consider a hollow spherical conductor with total charge \(+5 e\). The outer and inner radii are \(a\) and \(b,\) respectively. (a) Calculate the charge on the sphere's inner and outer surfaces if a charge of \(-3 e\) is placed at the center of the sphere. (b) What is the total net charge of the sphere?

A uniform sphere has a radius \(R\) and a total charge \(+Q\), uniformly distributed throughout its volume. It is surrounded by a thick spherical shell carrying a total charge \(-Q,\) also uniformly distributed, and having an outer radius of \(2 R\). What is the electric field as a function of \(R ?\)

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