Attenuation coefficient in metal in rectangular waveguide for transverse electric waves¶
A coaxial waveguide is an electrical cable consisting of a central conductor and a shield arranged coaxially and separated by an insulating material or an air gap. It is used to transmit radio frequency electrical signals. The specific resistance of a coaxial waveguide depends on the radius of the outer conductor and the radius of the inner conductor, as well as on the relative permeability of the insulator material, frequency of signal and specific conductivity of conductor.
Conditions:
Waves propagating in the waveguide must be transverse electric waves.
Second index \(n \ge 1\).
- attenuation_coefficient¶
attenuation_coefficientin metal.
- Symbol:
alpha- Latex:
\(\alpha\)
- Dimension:
1/length
- surface_resistance¶
electrical_resistanceof the surface.
- Symbol:
R_s- Latex:
\(R_\text{s}\)
- Dimension:
impedance
- first_index¶
The first index shows how many half-wavelengths fit across the width of the cross section.
- Symbol:
m- Latex:
\(m\)
- Dimension:
dimensionless
- second_index¶
The second index shows how many half-wavelengths fit across the height of the cross section.
- Symbol:
n- Latex:
\(n\)
- Dimension:
dimensionless
- Symbol:
a- Latex:
\(a\)
- Dimension:
length
- Symbol:
b- Latex:
\(b\)
- Dimension:
length
- medium_resistance¶
electrical_resistanceof the medium filling the waveguide.
- Symbol:
R- Latex:
\(R\)
- Dimension:
impedance
- wavelength¶
wavelengthof the signal.
- Symbol:
lambda- Latex:
\(\lambda\)
- Dimension:
length
- critical_wavelength¶
Critical
wavelengthof the system. See Critical wavelength of waveguide.
- Symbol:
lambda_c- Latex:
\(\lambda_\text{c}\)
- Dimension:
length
- law¶
alpha = 2 * R_s / R / (a * sqrt(1 - (lambda / (2 * lambda_c))^2)) * ((1 + a / b) * (lambda / (2 * lambda_c))^2 + (1 - (lambda / (2 * lambda_c))^2) * a / b * (a / b * n^2 + m^2) / ((a / b * n)^2 + m^2))- Latex:
- \[\alpha = \frac{2 \frac{R_\text{s}}{R}}{a \sqrt{1 - \left(\frac{\lambda}{2 \lambda_\text{c}}\right)^{2}}} \left(\left(1 + \frac{a}{b}\right) \left(\frac{\lambda}{2 \lambda_\text{c}}\right)^{2} + \frac{\left(1 - \left(\frac{\lambda}{2 \lambda_\text{c}}\right)^{2}\right) \frac{a}{b} \left(\frac{a}{b} n^{2} + m^{2}\right)}{\left(\frac{a}{b} n\right)^{2} + m^{2}}\right)\]