1 / 32

Prof. David R. Jackson Dept. of ECE

ECE 5317-6351 Microwave Engineering. Fall 2011. Prof. David R. Jackson Dept. of ECE. Notes 4. Waveguides Part 1: General Theory . Waveguide Introduction . In general terms, a waveguide is a devise that confines electromagnetic energy and channels it from one point to another. Examples.

ataret
Download Presentation

Prof. David R. Jackson Dept. of ECE

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. ECE 5317-6351 Microwave Engineering Fall 2011 Prof. David R. Jackson Dept. of ECE Notes 4 Waveguides Part 1: General Theory

  2. Waveguide Introduction In general terms, a waveguide is a devise that confines electromagnetic energy and channels it from one point to another. Examples • Coax • Twin lead (twisted pair) • Printed circuit lines • (e.g. microstrip) • Optical fiber • Parallel plate waveguide • Rectangular waveguide • Circular waveguide Note: In microwave engineering, the term “waveguide” is often used to mean rectangular or circular waveguide (i.e., a hollow pipe of metal).

  3. General Solutions for TEM, TE and TM Waves Assume ejt time dependence and homogeneous source-free materials. Assume wave propagation in the  z direction transverse components

  4. Helmholtz Equation Vector Laplacian definition : where

  5. Helmholtz Equation Assume Ohm’s law holds:

  6. Helmholtz Equation (cont.) Next, we examine the term on the right-hand side.

  7. Helmholtz Equation (cont.) To do this, start with Ampere’s law: In the time-harmonic (sinusoidal steady state, there can never be any volume charge density inside of a linear, homogeneous, isotropic, source-free region that obeys Ohm’s law.

  8. Helmholtz Equation (cont.) Hence, we have Helmholtz equation

  9. Helmholtz Equation (cont.) Similarly, for the magnetic field, we have

  10. Helmholtz Equation (cont.) Hence, we have Helmholtz equation

  11. Helmholtz Equation (cont.) Summary Helmholtz equations These equations are valid for a source-free homogeneous isotropic linear material.

  12. Field Representation Assume a guided wave with a field variation in the z direction of the form Then all six of the field components can be expressed in terms of these two fundamental ones:

  13. Field Representation (cont.) Types of guided waves: TEMz • TEMz:Ez = 0, Hz = 0 w • TMz:Ez0, Hz = 0 er h • TEz:Ez = 0, Hz 0 Microstrip TMz,TEz • Hybrid:Ez0, Hz 0 Hybrid

  14. Field Representation: Proof Assume a source-free region with a variation

  15. Field Representation: Proof (cont.) Combining 1) and 5) Cutoff wave number A similar derivation holds for the other three transverse field components.

  16. Field Representation (cont.) Summary These equations give the transverse field components in terms of longitudinal components, Ezand Hz.

  17. Field Representation (cont.) Therefore, we only need to solve the Helmholtz equations for the longitudinal field components (Ez and Hz).

  18. Transverse Electric (TEz) Waves The electric field is “transverse” (perpendicular) to z. In general, Ex,Ey,Hx,Hy,Hz  0 To find the TEzfield solutions (away from any sources), solve

  19. Transverse Electric (TEz) Waves (cont.) Recall that the field solutions we seek are assumed to vary as Solve subject to the appropriate boundary conditions. (This is an eigenvalue problem.)

  20. Transverse Electric (TEz) Waves (cont.) Once the solution for Hz is obtained, For a wave propagating in the positive z direction (top sign): For a wave propagating in the negative z direction (bottom sign): TE wave impedance

  21. Transverse Electric (TEz) Waves (cont.) Also, for a wave propagating in the positive z direction, Similarly, for a wave propagating in the negative z direction,

  22. Transverse Magnetic (TMz) Waves In general, Ex,Ey,Ez,Hx,Hy 0 To find the TEzfield solutions (away from any sources), solve

  23. Transverse Magnetic (TMz) Waves (cont.) solve subject to the appropriate boundary conditions (Eigenvalue problem)

  24. Transverse Magnetic (TMz) Waves (cont.) Once the solution for Ezis obtained, For a wave propagating in the positive z direction (top sign): For a wave propagating in the negative z direction (bottom sign): TM wave impedance

  25. Transverse Magnetic (TMz) Waves (cont.) Also, for a wave propagating in the positive z direction, Similarly, for a wave propagating in the negative z direction,

  26. Transverse ElectroMagnetic(TEM) Waves In general, Ex,Ey,Hx,Hy 0 From the previous equations for the transverse field components, all of them are equal to zero if Ezand Hz are both zero. Unless (see slide 16) For TEM waves Hence, we have

  27. Transverse ElectroMagnetic(TEM) Waves (cont.) In a linear, isotropic, homogeneous source-free region, In rectangular coordinates, we have Notation:

  28. Transverse ElectroMagnetic(TEM) Waves (cont.) Also, for the TEMz mode we have from Faraday’s law (taking the z component): Taking the z component of the curl, we have Notation: Hence or

  29. Transverse ElectroMagnetic(TEM) Waves (cont.) Hence

  30. Transverse ElectroMagnetic(TEM) Waves (cont.) Since the potential function that describes the electric field in the cross-sectional plane is two dimensional, we can drop the “t” subscript if we wish: Boundary Conditions: a b This is enough to make the potential function unique. Hence, the potential function is the same for DC as it is for a high-frequency microwave signal.

  31. Transverse ElectroMagnetic(TEM) Waves (cont.) • Notes: • A TEMz mode has an electric field that has exactly the same shape as a static (DC) field. (A similar proof holds for the magnetic field.) • This implies that the C and L for the TEMz mode on a transmission line are independent of frequency. • This also implies that the voltage drop between the two conductors of a transmission line carrying a TEMz mode is path independent. • A TEMz mode requires two or more conductors (a static field cannot be supported by a single conductor such as a hollow metal pipe.

  32. TEM Solution Process A) Solve Laplace’s equation subject to appropriate B.C.s.: B) Find the transverse electric field: C) Find the total electric field: D) Find the magnetic field:

More Related