Example24 Waveguide-to-Coaxial Adapter

General

  • The characteristics of a waveguide-to-coaxial adapter are analyzed.
     

  •  

  • Unless specified in the list below, the default conditions will be applied.
     

Analysis Conditions

The harmonic analysis is set as follows.

Tab

Setting Item

Settings

Mesh Tab

Frequency-Dependent Meshing

Reference frequency: 1×10^10[Hz]

Select “The conductor bodies thicker than the skin depth constitute the boundary condition.”

 

Harmonic analysis

Frequency

Minimum: 8×10^9[Hz]

Maximum: 15×10^9[Hz]

Sweep Type

Select Linear step

Division number: 7

Sweep Setting

Select Discrete sweep

Input

1.0[W]

 

Model

The model is a waveguide-to-coaxial adapter. The inner conductor of coaxial cable is penetrated into the circular waveguide.

 

 

 

Body Attributes and Materials

Body Number/Type

Body Attribute Name

Material Name

7/Solid

InnerConductor

003_Ag *

8/Solid

Waveguide

000_Air(*)

9/Solid

Resin

Resin

* Available from the Material DB

 

 

The material properties of Resin are set up as follows:

Material Name

Tab

Properties

DRMat

Permittivity

Relative permittivity: 2.3

 

Boundary Conditions

Boundary Condition Name/Topology

Tab

Boundary Condition Type

Settings

Port_001/Face

 

Electric

 

I/O Port

 

Reference Impedance: Select “Specify”

and enter 50 ohms.

Number of Modes

Number of precalculated modes: 5

Number of modes used in the actual analysis: 1

Select modes: none

Port_002/Face

Electric

I/O Port

Reference Impedance: Select
“Use the characteristic impedance calculated from the port structure”

and enter 50[ohm].

Number of Modes

Number of precalculated modes: 5

Number of modes used in the actual analysis: 2

Select modes: none

Outer Boundary Condition

Electric

Electric wall

 

 

Notes:

Number of modes used in the actual analysis is 2 for Port_002.

This is because there are two TE11 modes.

The directions of their electric field vectors are angled 90 degrees each other.

Both modes need to be taken into account for correct analysis. Femtet cannot control mode’s direction at the moment.

Results

Ports have been set as follows.

 

Port_001 Number of modes used in the actual analysis: 1

Port_002 Number of modes used in the actual analysis: 2

 

Therefore, S-parameters are a 3 x 3 matrix.

 

 

 

S-parameters

 

On the Results tab, click [Chart] – [SYZ Matrix]. The following will appear.

 

Port Index
1:Port_001:m1
2:Port_002:m1
3:Port_002:m2

 

 

“m1” and “m2” indicate the mode number.

See [How to Examine the Ports of Electromagnetic Analysis] for the detail.

 

 

 

Two TE11 modes

 

The first propagation constant dialog box above shows the following:

 

(This dialog box appears when you click [Chart] – [Mode Information] on the Results tab )

 

Port_002 p2m1: 9.691647e+001 +j 0.000000e+000

 

This is for Port_002:m1 of Port Index.

Note that “p” is for port and “m” is for mode in p2m1. The second “propagation constant” dialog box shows the following:

 

Port_002 p2m2: 9.681297e+001 +j 0.000000e+000

 

This is for Port_002:m2 of Port Index.

 

The power entered at Port_001 reaches Port_002 in these two modes.

The total power is acquired by the following equation.

Please use Excel or any other tool to calculate it. Femtet doesn’t calculate this equation.

 

(1)

 

A TM01 mode also exists at 12[GHz] or higher. For better accuracy at 12[GHz] or higher,

increase “Number of modes used in the actual analysis” for Port_002 from 2 to 3.

 

 

The TM0-mode electric field distribution (at 12GHz)