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Presentation on theme: "EE3321 ELECTROMAGENTIC FIELD THEORY"— Presentation transcript:

Week 4 Gauss’ Law, Flux Density Gaussian Surface Electric Potential Poisson’s Equation

2 Gauss’ Law As it turns out, Coulomb's law is actually a special case of Gauss' Law, a more fundamental description of the relationship between the distribution of electric charge in space and the resulting electric field. Gauss's law is one of Maxwell's equations, a set of four laws governing electromagnetics. The law bears the name of Karl Friedrich Gauss ( ), one of the greatest mathematicians of all time who also made significant contributions to theoretical physics.

3 Differential form of Gauss’ Law
In differential form, Gauss' law states that the divergence of the E field is proportional to the charge density that produces it: where ρ is the total electric charge density (in units of C/m³) єo is the electric constant (8.854 x 10-12 F/m)

4 Exercise Suppose that a charge is distributed in a sphere of radius R =1 m. In the region 0 < R < 1 m the electric field is given by E = 1 x 10 – 6 R aR. Find the charge density in this region. Recall the expression for the divergence in spherical coordinates. Find the charge density for R< 1 m Plot the charge density as a function of R.

5 Integral form of Gauss’ Law
We can make use of the divergence theorem to obtain the integral form of Gauss’s law: where Q is the charge enclosed by the surface of integration and is equal to the volume integral of the charge density.

6 Flux Density We define the electric flux density as
Then, the electric flux is given by

7 Electric Dipole Consider the case of an electric dipole. What is the total flux coming out of the rectangular surface?

8 Gaussian Surface A Gaussian surface is a closed two-dimensional surface through which a flux or electric field is to be calculated. The surface is used in conjunction with Gauss's law, allowing one to calculate the total enclosed electric charge by performing a surface integral. Gaussian surfaces are usually carefully chosen to exploit symmetries of a situation to simplify the calculation of the surface integral. If the Gaussian surface is chosen such that for every point on the surface the component of the electric field along the normal vector is constant, then the calculation will not require difficult integration as the constant can be pulled out of the integration sign.

9 Spherical Surface A spherical Gaussian surface is used when finding the electric field or the flux produced by any of the following: a point charge a uniformly distributed spherical shell of charge any other charge distribution with spherical symmetry The spherical Gaussian surface is chosen so that it is concentric with the charge distribution.

10 Point Electric Charge What is the total flux out of a spherical surface around a point charge? What is the divergence of D?

11 Exercise Let D = Do R aR for R≤ a. Determine the amount of charge enclosed by a spherical surface of radius b for: b<a b=a b>a 

12 Exercise Consider a charged spherical shell of negligible thickness, with a uniformly charge density ρs and radius a. Use Gauss's law to find the magnitude of the resultant electric field E inside the charged shell.

13 Tesla Cage In a Tesla cage, the net flux is zero and the magnitude of the electric field is also zero.

14 Cylindrical Gaussian Surface
A cylindrical Gaussian surface is used when finding the electric field or the flux produced by an infinitely long line of uniform charge.

15 The Pillbox This Gaussian surface is used to find the electric field due to an infinite plane of uniform charge.

16 Electric Potential The electrical potential difference is defined as the amount of work needed to move a unit electric charge from the second point to the first, or equivalently, the amount of work that a unit charge flowing from the first point to the second can perform. The potential difference between two points A and B is the line integral of the electric field E

17 Line Integral The integration path is an arbitrary path connecting point A of known potential to the observation point B as shown below. The value of V is independent of the integration path.

18 Line Integral The value of V is independent of the integration path.

19 Exercise Let E = Eo az (V/m) for z>0. Find the potential between the points A and B: A = (0, 0, 0) and B = (1, 1, 1) Steps: set up the integral following a simple path A to (1, 0, 0) (1, 0, 0) to (1, 1, 0) (1, 1, 0) to B

20 Potential at Infinity The potential at infinity is said to be zero.
If a test charge +q moves toward a charge +Q starting at an infinite range it will gain potential at point P.

21 Gradient of V When the magnetic field is constant in time, it is possible to express the electric field as the gradient of the electrostatic potential.

22 Exercise A spherically charged shell of radius a, centered at the origin, creates the potential V = – Voa/R (Volts) for R>a. Determine the corresponding electric field E. Recall the expression of the gradient operator in spherical coordinates. Notice that the potential V is independent of the azimuth and elevation angles.

23 Exercise Consider the potential V = 4 ln ( a/r ) in cylindrical coordinates. Find E. Recall the expression for the gradient operator in cylindrical coordinates. Notice that the potential V is independent of the azimuth angle and the elevation z.

24 Equipotential Lines and Surfaces
An equipotential line is a line in space where the potential is constant. An equipotential surface is a surface in space where the potential is constant. No work is required for a charge to move along an equipotential surface. Work is required for a charge to move to a different equipotential surface.

25 Point Charge For a point charge, an equipotential line takes the shape of a circle, and an equipotential surface is a sphere centered on the charge.

26 Capacitor Consider two large parallel plates separated by a short distance L. Assuming that the plates have a uniform charge distribution, the electric field lines are perpendicular to the plates and the equipotential lines are parallel to the plates.

27 Potential Well If a test charge approaches the charged sphere it will experience a decreasing potential. The potential is symmetric and decreases as the observation gets closer to the sphere. The concentric orbits in the figure represent lines of equal potential.

28 Poisson’s Equation Poisson's equation relates the potential V to the charge density ρ. To determine V one needs to make use of boundary conditions. If the charge density is zero, then Laplace's equation results. Cathode Tube

29 Exercise Let d2V/dz2 = 0 with boundary conditions V(0) = 0 and V(z=d)=100 V. Find for V(z). Integrate Laplace’s Equation over z. Integrate again. Apply boundary conditions.

30 Homework Read sections 4-4 and 4-5
Solve the following end-of-chapter problems: 4.22, 4.24, 4.28, 4.30, 4.34

31 Review “Hyperphysics”


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