JPS56147501A - Wave type waveguide for short millimeter and submillimeter wave - Google Patents
Wave type waveguide for short millimeter and submillimeter waveInfo
- Publication number
- JPS56147501A JPS56147501A JP4958980A JP4958980A JPS56147501A JP S56147501 A JPS56147501 A JP S56147501A JP 4958980 A JP4958980 A JP 4958980A JP 4958980 A JP4958980 A JP 4958980A JP S56147501 A JPS56147501 A JP S56147501A
- Authority
- JP
- Japan
- Prior art keywords
- electromagnetic
- horn
- component
- aperture
- attenuation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000004020 conductor Substances 0.000 abstract 2
- 230000005672 electromagnetic field Effects 0.000 abstract 2
- 230000005684 electric field Effects 0.000 abstract 1
- 230000000644 propagated effect Effects 0.000 abstract 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P3/00—Waveguides; Transmission lines of the waveguide type
- H01P3/12—Hollow waveguides
Landscapes
- Waveguides (AREA)
Abstract
PURPOSE:To reduce attenuation, by making the electromagnetic field at guide wall small, periodically changing the guide diameter in the direction of guide axis, and changing the area of aperture of energizing electromagnetic horn of multimode waveguide so that the phase speed of each mode can be equal to the light speed. CONSTITUTION:The section of the input section A consists of the aperture of the electromagnetic cone horn 2 and the conductor plate, and the surface component of the electric field shows the same distribution as the main waves at the aperture of the horn 2 and it is zero at the conductor surface according to the boundary condition. The distribution in the section is a little distored since all the modes are propagated in the light speed, but they are propagates axially with almost the same sectional distribution. The sectional component of the electromagnetic field near the guide wall is very little. It is smaller when the area of the electromagnetic horn 2 for energizing is smaller, and the axial component of the magnetic field is negligibly small for the spherical waveguide to the sectional component. Thus, the attenuation can be made the same as or lower than the attenuation of the magnetic type axial mode of the circular type waveguide 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4958980A JPS56147501A (en) | 1980-04-17 | 1980-04-17 | Wave type waveguide for short millimeter and submillimeter wave |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4958980A JPS56147501A (en) | 1980-04-17 | 1980-04-17 | Wave type waveguide for short millimeter and submillimeter wave |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS56147501A true JPS56147501A (en) | 1981-11-16 |
Family
ID=12835408
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4958980A Pending JPS56147501A (en) | 1980-04-17 | 1980-04-17 | Wave type waveguide for short millimeter and submillimeter wave |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56147501A (en) |
-
1980
- 1980-04-17 JP JP4958980A patent/JPS56147501A/en active Pending
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