Course Overview
Course: Engineering Electromagnetics
Instructor: Mohamed Fareq Malek
University: UOWD
Focus: Lecture 3 discusses Capacitance, Poisson’s Equations, Steady Magnetic Field, and Maxwell’s Equations for Static Fields.
References
Primary Reference: W.H. Hayt Jr. and J. A. Buck
Chapters covered: 6, 7, 8
Outline covered in the lecture:
Capacitance
Poisson’s Equations
Steady Magnetic Field
Maxwell’s Equations for Static Fields
3.1 Capacitance
Definition: Capacitance quantifies the ability of a device to store electrical energy.
Basic Structure of a Capacitor:
Comprises two oppositely charged conductors separated by a dielectric material.
Capacitance Formula:
C = \frac{Q}{V_0} where:
C = Capacitance (in Farads)
Q = Stored Charge
V_0 = Applied Voltage
Stored Energy in a Capacitor:
Energy stored is dependent on capacitance and voltage.
Steps to Calculate Capacitance (D. Cheng)
Select a suitable coordinate system based on the geometry of the capacitor.
Assume charges +Q and -Q on conductors.
Calculate the electric field (E).
Evaluate the potential difference (V_0).
Determine the capacitance ratio.
Calculation example provided:
For a coaxial transmission line:
Assumes hollow inner conductor with equal and opposite charges on inner and outer conductors.
The electric field E is zero elsewhere.
Charge density on inner conductor is used to derive capacitance.
3.2 Poisson's Equations
Starting Point: Derived from Maxwell’s First Equation.
Formulation of Poisson’s Equation:
\nabla^2 V = -\frac{\rho}{\epsilon}
Purpose: Solves for potential field in a region when the electric field or potential values at boundaries are known.
Mathematical Concepts
Laplacian Operator:
Denoted as \nabla^2 (pronounced “del squared”). It represents the divergence of the gradient of a function.
In Cases of Zero Charge Density: Poisson’s equation simplifies to Laplace’s equation:
\nabla^2 V = 0.
Example: Parallel Plate Capacitor
Assumption: Plate separation (d) much smaller than plate dimensions.
Laplace’s equation changes based on this simplification; after integration, boundary conditions yield:
V(x=0) = 0,
V(x=d) = V_0.
3.3 Steady Magnetic Field
Definition: Magnetic Field (H) generated by currents in circuits.
Biot-Savart Law: Predicts magnetic field intensity (H) based on a point source current element (dL):
[H] = A/m.
Key Concept: Models forces between currents effectively regardless of their orientations.
Definitions & Applications
Magnetic Flux Density: Measures the magnetic field strength, expressed in Weber/m² or Tesla.
Ampere’s Circuital Law
Statement: The line integral of H around a closed path equals the current I enclosed.
Independent of material properties and path choice.
Application: For cylindrical coordinates around an infinite wire, we expect magnetic field intensity H to vary only with the radial distance (r).
Example: Coaxial Transmission Line
Configuration: Two concentric conductors carrying equal and opposite currents (I).
Goal: Find magnetic field for all radial distances (r).
Expressions derived for different radial regions:
For 0 < r < a: Field decreased by a factor of radius,
For a < r < b: Field proportional to the total current,
For r > c, total current enclosed is zero.
3.4 Maxwell's Equations for Static Fields
Context: Foundational theory underlying electrostatics and magnetostatics.
Mathematical Concepts
Divergence and Curl:
Divergence indicates the source strength of an electric field, and curl describes circulation strength of a magnetic field.
Curl Definition: Describes the rotation of a vector field.
Given by:
\text{Curl} \vec{F} = \nabla \times \vec{F}
Computation of Curl: In rectangular coordinates, it involves cross products.
Coordinate System Formulation
Cylindrical Coordinates: Describes transformation of vector fields based on different geometric configurations.
Spherical Coordinates: Similar to cylindrical but adapted for spherical symmetry.
Notable Examples
Provided Example for Currents: Calculated curl in relation to a given magnetic field.
Maxwell’s Equations Final Form: For static fields in point form:
Gauss’ Law for electric fields,
Conservative property of the static electric field,
Ampere’s Circuital Law,
Gauss' Law for magnetic fields.
Integration over regions yields various integral forms, extending implications for dynamics and time-varying fields in future discussions.