Chapter 2: Electric Fields

2.1 Introduction to Electric Fields

Electric fields are all around us. An electric field is a region surrounding a charged object where another charged object experiences a force due to electrostatic attraction or repulsion. The electric field (\vec{E}) is a vector quantity, meaning it has both magnitude and direction.

The electric field is defined as the force per unit charge that a test charge would experience at a specific point in the field.

2.2 Electric Field due to a Point Charge

The electric field due to a point charge (q) can be calculated using the following formula:

E = k \dfrac{|q|}{r^2}

where E is the magnitude of the electric field, k is the electrostatic constant (approximately 8.99 \times 10^9 \text{ N} \cdot \text{m}^2 / \text{C}^2), q is the charge of the source, and r is the distance from the charge to the point in the field.

The direction of the electric field is radially outward for positive charges and radially inward for negative charges.

The electric field can also be expressed as:

\vec{E} = \dfrac{\vec{F}}{q}

The unit of the electric field is newtons per coulomb (N/C) or volts per meter (V/m). These two units are totally equivalent such that 1 \frac{N}{C} = 1 \frac{V}{m}.

2.3 Superposition of Electric Fields

When multiple charges are present, the net electric field at a specific point is the vector sum of the electric fields due to each individual charge. This principle is known as superposition and is applicable to electric fields as it is to forces.

To apply the superposition principle, simply define a coordinate system and break each electric field vector into components (be sure to assign positive and negative values according to the way you drew your coordinate system). Suppose you choose an X-Y coordinate system. Start by summing up all of the x components separately from the y components. You will be left with the net x component and the net y component. Add these components together (using the rules of vector addition), and the resultant vector will point in the direction of the electric field.

2.4 Electric Field Lines

Electric field lines provide a visual representation of the electric field. They indicate the direction of the electric field at any point and are tangent to the field at that point. Field lines start at positive charges and end at negative charges. The density of field lines is proportional to the field’s strength.

2.5 Conductors in Electric Fields

In a conductor, charges can move freely. When a conductor is placed in an electric field, charges redistribute themselves on the surface until the electric field inside the conductor is zero. This phenomenon is known as electrostatic shielding.

2.6 Electric Flux

Electric flux (\Phi) is a measure of the number of electric field lines passing through a given surface. Mathematically, electric flux is the dot product of the electric field (\vec{E}) and the vector area (\vec{A}) of the surface:

\Phi_E = \vec{E} \cdot \vec{A} = |\vec{E}| |\vec{A}| \cos(\theta)

where \theta is the angle between the electric field and the vector pointing normal to the surface (\vec{A}). In the next chapter, we will discuss electric flux in more detail.

Chapter Summary

In this chapter, we have covered the basic concepts of electric fields, including their definition, calculation, and representation using field lines. We have also discussed the superposition principle for electric fields and the concept of electric flux. These ideas will serve as the foundation for understanding more complex topics in electricity and magnetism throughout this course.

Continue to Chapter 3: Electric Flux

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