What is a Waveguide?

What is a Waveguide? How do signals propagate in waveguides? What are TE and TM operation modes?

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- everything RF

Jan 20, 2025

A Waveguide is a specialized structure that is used to direct electromagnetic waves from one point to another with minimal signal loss, at high frequencies. Unlike the traditional transmission lines, waveguides do not have a central conductor. Instead, they are hollow and rely on the reflections from the inner walls of the tube to guide the waves and transmit power from one point to another. They are widely used in microwave and RF communications, optical systems, and radar applications. 

Rigid Rectangular Waveguide (WG00 to WG27 / WR2300 to WR10) – Global  Invacom GroupA rigid rectangular waveguide 

The structure of the waveguide is an important parameter that determines how the wave will propagate through it. It makes the waveguide highly efficient for high-frequency signals. Waveguides are generally hollow metallic tubes or dielectric structures with retangular, circular or elliptical cross-sectional shape. The metallic waveguides have conductive walls which help in reflecting the electromagnetic waves, whereas in the dielectric waveguides a high-refractive index core is surrounding by a lower-index cladding for total internal reflection of the signal.

Waveguides can be classified based on a lot of parameters like waveguide shape, size, flange, structure, material, operating mode, frequency of operation, etc.

Key Physical Parameters of Waveguides

Waveguide Flange: The connection interface of a waveguide is called a Waveguide Flange. It is used to connect sections of waveguides or interface waveguides with other components, such as antennas, test equipment, or other waveguide sections. Click here to learn more about waveguide flanges.

undefinedFlange for a rectangular waveguide

Waveguide Shape: The waveguides are classified as rectangular and circular. The rectangular waveguides have cross-section of rectangular shape and circular waveguides have a cross-section that is circular in shape.

Waveguide Size: Waveguide components are available in various sizes. To function properly the waveguide must have a certain minimum cross section, relative to the wavelength of the signal. If the wavelength of the signal is too long compared to the cross-sectional area the waveguide the signal will not be able to propagate. There are a set of standard waveguide sizes that have been developed. Click here to see all the standard waveguide sizes.

Rigid/Flexible Waveguides: The tube of the waveguide section is usually made of a metal material that is rigid and can not bend, however flexible waveguide tubes are also available. The flexible nature makes them more adaptable to scenarios where some movement is expected between two connected systems.

Standard & Ridged Waveguides: In order to alter the electromagnetic properties of the waveguides, ridges (raised or protruding structures) can be added inside the waveguide along its broad wall and run parallel to the direction of propagation of wave. See an example below. The addition of a ridge can alter the cutoff frequency of the waveguide. Click here to read more about Ridged Waveguides.

 

Modes of Operation

In waveguide theory, the terms TE (Transverse Electric) and TM (Transverse Magnetic) refer to the two primary operating modes of electromagnetic waves propagating through a waveguide. These modes define the behavior of the electric and magnetic fields inside the waveguide and determine how the wave travels through it.

Transverse Electro-Magnetic (TEM)Transverse directions w.r.t the direction of signal propagation in a Waveguide 

TE Mode (Transverse Electric Mode) 

In TE mode, the electric field is entirely transverse to the direction of propagation (see image above), meaning it has no component along the direction of the wave propagation, whereas the magnetic field will have components in all three directions, including the direction of propagation of wave. There are infinite number of solutions for the wave equation corresponding to the magnetic fields. The solutions are disguised using the mode indexes, and the modes are represented as TE(m,n), where ‘m’ represents the number of half-wavelength variations of the electric field along the x-direction and ‘n’ represents the number of half-wavelength variations of the electric field along the y-direction. The ‘m’ and ‘n’ values can be 0,1,2.. and must satisfy the relationship m ≠ n. Each mode is associated with a cut-off frequency, below which no TE propagation occurs in rectangular waveguides. The mode of propagation with the lowest cut-off frequency is called the dominant mode. TE10 is the dominant mode in rectangular waveguides.  

6 meanings of Te and TM in rectangular waveguide - DOLPH MICROWAVEDifferent TE modes showing the variations in electric filed with change in value of ‘m’  

TM Mode (Transverse Magnetic Mode) 

In TM mode, the magnetic field has no component in the direction of propagation, meaning it is entirely transverse to the direction of propagation, i.e. it lies in the cross-sectional plane of the waveguide. Whereas the electric field has component along the direction of propagation (the waveguide axis). When Maxwell’s equation or wave equation for the electric fields in the rectangular waveguide is solved, and infinite solutions can be distinguished using the mode indexes. The value of m or n can never be equal to zero, but unlike TE mode, m can be equal to n, making the dominant mode in the rectangular waveguide is TM11. 

 undefinedTM11 Mode

The lowest operating mode in a rectangular waveguide is the TE10 mode and the cutoff frequencies of the TE and TM mode depend on the dimension of the waveguide. In a circular waveguide, the cross-section of the waveguide is circular. They support both the TE and TM modes, but typically allow more complex mode patterns as compared to rectangular waveguides. The dominant mode in circular waveguides is often the TE11 mode, while higher-order models can also propagate.

Characteristics of Waveguides 

1. Cutoff Frequency of Waveguides: The cutoff frequency for each mode in a waveguide is the specific frequency, below which the mode cannot propagate. This frequency is determined by the waveguide’s dimensions and the mode of operation. For rectangular waveguides, the cutoff frequency fc for the dominant TE10 mode can be calculated by the equation below. You can also use our calculator to calculate the cutoff frequency for rectangular waveguides.

 

For circular waveguides, the cutoff frequency fc  for the dominant mode can be calculated by the equation below. You can also use our calculator to calculate the cutoff frequency for circular waveguides.



Click here to learn more about Waveguide Cutoff Frequencies

2. Impedance and Losses: The characteristic impedance of a waveguide depends on the operating mode and the frequency. As the frequency increases, the impedance changes, which affects the efficiency of the energy transfer. There are two loss mechanisms that occur in the waveguides - conductor losses and dielectric losses.

Conductor losses occur due to surface resistance in the waveguide walls, which is more visible at high frequencies. Dielectric losses are found in dielectric-filled waveguides, where the energy is absorbed by the material. 

3. Phase Velocity: The phase velocity refers to the speed at which a specific phase of a wave (e.g., a crest) propagates through a medium. The phase velocity of waves in a waveguide may be higher than the speed of light in free space. However, this does not violate the principles of relativity, as the group velocity, which represents the speed at which the overall shape or the envelope of the wave (carrying energy or information) moves, is below the speed of light.

 The phase velocity is given as:

where λc is the wavelength of light.

4. Wavelength: In a waveguide the effective wavelength of an electromagnetic wave differs from its free-space wavelength due to the constraints imposed by the geometry of waveguide. This difference is explained by the phase velocity and cutoff frequency which lead to a longer wavelength inside the waveguide. This effect becomes significant as the operating frequency approaches the waveguide’s cutoff frequency.

Where λg is the waveguide wavelength, λo is the free-space wavelength, and ‘a’ is the broad dimension of the waveguide.

- Retired

Jan 19, 2025

My professor in collage explained how waveguides were invented, as he was a US Navy Electronics Technician after WW!!. When RADAR was first installed on Navy ships, they ran the RF transmission lines up the mast to the RADAR dish that would rotate and search for enemy ships on the horizon. It worked well, but there was a problem. The RF transmission lines were attached to the mast with porcelain insulators, which worked great, until the guns had to be fired, which happened anytime the ship was in battle. As soon as the guns were fired, the mast would whip back and forth and snap the insulators, which would cause the transmission lines to short out, causing the magnetron in the transmitter to fail. So the ship's captain had to be very careful to not fire the ship's guns until the last minute, because as soon as he fired the first shot, the RADAR would go down and he would be blind for the rest of the battle.

This was an unacceptable situation, so they went looking for a solution. Porcelain insulators were too fragile to use on the mast, so they looked into other options. Then somebody came up with a brilliant idea: Weld one quarter wavelength stubs to the mast and weld the RF transmission lines to the other end of the stubs, because one quarter wavelength from the mast (a dead short) is an open! So the stubs would be seen by the magnetron and the entire system as infinitely high impedance insulators, far less fragile than porcelain insulators. And now, if you add another quarter wavelength stub on the opposite side, and enclose it in a conductive sheet, you have a hollow tube that appears to pass the RF to the dish and nothing can short out of the transmission lines going up the mast, and exactly the same thing is happening on the other side at the mast. You now have a hollow tube running up the mast and nothing can short out the magnetron and you can fire the guns all day long with no ill effect, and with any luck, your ability to track the enemy during battle means you might just win the battle, and possibly the war. That is how waveguide came about, and that is how it works.