Electric field due to a charged disk

Explore the electric field due to a charged disk, its equation derivation, significance in electromagnetism, and an example calculation.

Understanding the Electric Field Due to a Charged Disk

In this article, we will explore the electric field generated by a uniformly charged disk, an essential concept in the study of electromagnetism. We will discuss the derivation of the equation and its significance without delving into specific calculations or numerical examples.

Derivation of the Electric Field Equation

The electric field produced by a charged disk can be determined using Gauss’s Law, which relates the electric field to the electric charge enclosed within a Gaussian surface. However, the symmetry of the charged disk requires us to apply the law differently. Instead of finding the electric field directly, we first determine the electric field produced by a charged ring, which is a subsection of the charged disk, and then integrate over the entire disk.

  1. Electric Field Due to a Charged Ring: Consider a charged ring with a uniform charge density λ and a radius R. Using Coulomb’s Law and integrating over the entire ring, we can derive the electric field produced by the ring at a point P, located along the axis perpendicular to the ring at a distance x from its center.
  2. Integrating Over the Charged Disk: The charged disk can be divided into an infinite number of concentric charged rings. To find the total electric field due to the disk, we integrate the electric field of each charged ring over the entire area of the disk. This requires us to express the charge density λ in terms of the surface charge density σ (charge per unit area) of the disk.

By performing the integration, we obtain the electric field due to a uniformly charged disk with surface charge density σ and radius R at a point P located along the axis perpendicular to the disk at a distance x from its center:

E = (σ/2ε₀) * (1 – (x/√(x² + R²)))

Significance of the Electric Field Equation

The derived equation for the electric field due to a charged disk is important in various applications, including the study of capacitors, electrostatic problems involving disks, and the design of certain electromagnetic devices.

  • Capacitors: The electric field equation is crucial for understanding parallel plate capacitors, where the charged disk can be considered as one of the plates.
  • Electrostatic Problems: In many electrostatic problems, the charged disk serves as a model for simplifying complex geometries, helping physicists to better understand the behavior of charged systems.
  • Electromagnetic Devices: The knowledge of electric fields produced by charged disks is also vital in designing and optimizing various electromagnetic devices, such as sensors and actuators.

In conclusion, understanding the electric field due to a charged disk and its underlying equation is essential for anyone studying electromagnetism, as it has numerous applications and implications in the field.

Example Calculation: Electric Field Due to a Charged Disk

Let’s consider a charged disk with a radius R = 0.1 m and a uniform surface charge density σ = 5 × 10-6 C/m². We wish to find the electric field at a point P, located along the axis perpendicular to the disk at a distance x = 0.2 m from its center.

Using the equation derived earlier:

E = (σ/2ε₀) * (1 – (x/√(x² + R²)))

Where ε₀ is the vacuum permittivity, approximately equal to 8.854 × 10-12 C²/N·m².

Substitute the given values:

E = ((5 × 10-6 C/m²) / (2 * 8.854 × 10-12 C²/N·m²)) * (1 – (0.2 m / √((0.2 m)² + (0.1 m)²)))

First, let’s calculate the denominator inside the square root:

(0.2 m)² + (0.1 m)² = 0.04 m² + 0.01 m² = 0.05 m²

Now, calculate the square root:

√(0.05 m²) = 0.2236 m

Compute the fraction inside the parenthesis:

1 – (0.2 m / 0.2236 m) = 1 – 0.8951 = 0.1049

Finally, calculate the electric field:

E = ((5 × 10-6 C/m²) / (2 * 8.854 × 10-12 C²/N·m²)) * 0.1049 ≈ 2.97 × 105 N/C

Thus, the electric field at point P due to the charged disk is approximately 2.97 × 105 N/C.

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