Attenuation coefficient in metal¶
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 diameter of the outer conductor and the diameter of the inner conductor, as well as on the relative permeability and the relative permittivity of the insulator material, the surface resistance of the outer conductor and the surface resistance of the inner conductor.
- attenuation_coefficient¶
attenuation_coefficient
in metal.
- Symbol:
alpha
- Latex:
\(\alpha\)
- Dimension:
1/length
- relative_permittivity¶
relative_permittivity
of the insulator.
- Symbol:
epsilon_r
- Latex:
\(\varepsilon_\text{r}\)
- Dimension:
dimensionless
- relative_permeability¶
relative_permeability
of the insulator.
- Symbol:
mu_r
- Latex:
\(\mu_\text{r}\)
- Dimension:
dimensionless
- outer_surface_resistance¶
Surface
electrical_resistance
of the outer conductor.
- Symbol:
R_o
- Latex:
\(R_\text{o}\)
- Dimension:
impedance
- inner_surface_resistance¶
Surface
electrical_resistance
of the inner conductor.
- Symbol:
R_i
- Latex:
\(R_\text{i}\)
- Dimension:
impedance
- Symbol:
d_o
- Latex:
\(d_\text{o}\)
- Dimension:
length
- Symbol:
d_i
- Latex:
\(d_\text{i}\)
- Dimension:
length
- resistance¶
Constant equal to \(420 \Omega\).
- Symbol:
R_0
- Latex:
\(R_0\)
- Dimension:
impedance
- law¶
alpha = sqrt(epsilon_r / mu_r) * (R_i / d_i + R_o / d_o) / (pi * R_0 * log(d_o / d_i))
- Latex:
- \[\alpha = \frac{\sqrt{\frac{\varepsilon_\text{r}}{\mu_\text{r}}} \left(\frac{R_\text{i}}{d_\text{i}} + \frac{R_\text{o}}{d_\text{o}}\right)}{\pi R_0 \log \left( \frac{d_\text{o}}{d_\text{i}} \right)}\]