Читать книгу Introduction To Modern Planar Transmission Lines - Anand K. Verma - Страница 132

Figure (3.27a) shows the shunt inductor loaded line structure. An infinitesimally small Δx line length is considered. The cascading of a large number line sections, under the condition Δx → 0, forms a continuous line. The standard Δx long host transmission line section is modeled by the distributed line constants L and C p.u.l. The host line section is loaded with the inclusion, i.e. with additional shunt inductance L_sh. The loading element, i.e. inclusion is shown in the gray box, so the periodic embedding of reactive inclusion in the host line medium creates an artificial 1D mixture medium. The concept of the mixture material is further discussed in subsection (6.3.1) of chapter 6.

The inclusion lumped shunt inductance L_sh distributed over the length Δx is (L_sh/Δx) p.u.l. The total series inductance, (L Δx), gives the total series impedance Z = j ωL Δx and a combination of shunt capacitance (C Δx) and shunt inductance (L_sh/Δx) gives the total shunt admittance, Y = j (ωCΔx − Δx/(ωL_sh)). The transmission line equations for the shunt inductor loaded line are obtained as follows:

(3.4.1)

For the limiting case, Δx → 0, Δt → 0, the following expressions are obtained:

(3.4.2)

The voltage v across the shunt inductor is

(3.4.3)

From equation (3.4.2a,b), the following voltage wave equation is obtained:

(3.4.4)

On substituting ∂i₂/∂t from equation (3.4.3) in the above equation, the above wave equation is reduced to

(3.4.5)

where is the phase velocity of the standard nondispersive line without shunt loaded inductance, i.e. for the case L_sh → ∞. For a line in the air medium, the phase velocity is the velocity of the EM‐wave in a vacuum, i.e. v₀ = c. The cut‐off frequency is defined as . Finally, the above voltage wave equation of the dispersive transmission line is rewritten as

(3.4.6)

Equation (3.4.6) is known as the Klein–Gordon equation [B.20]. For a line without cut‐off frequency, i.e. for ω_c = 0, the above equation is reduced to the standard dispersionless transmission line equation (2.1.24) of chapter 2. On assuming the harmonic solution for the forward‐moving voltage, the voltage on the loaded line is

(3.4.7)

On substituting equation (3.4.7) in equation (3.4.6), the following dispersion relation is obtained:

(3.4.8)

Equation (3.4.8) is identical to equation (3.3.8a) for the plasma medium. The cut‐off frequency ω_c of the loaded line corresponds to the plasma frequency ω_p. Thus, a plasma medium can be modeled by the shunt inductor loaded transmission line. Further, Fig (3.27a) shows that below the cut‐off frequency, i.e. for ω < ω_c the circuit is reduced to the L‐L circuit presenting inductors in both the series and shunt arm. Such a medium is called the epsilon negative (ENG) medium, discussed in section (5.5) of chapter 5.

For frequency ω < ω_c, the propagation constant β is the imaginary quantity and the voltage wave cannot propagate on the shunt inductor loaded line. The voltage wave propagates only for ω > ω_c. Thus, the shunt inductor loaded line behaves like a high‐pass filter (HPF). It is like a metallic waveguide discussed in subsection (7.4.1) of chapter 7. For ω < ω_c, the loaded line supports the nonpropagating attenuated wave, called the evanescent wave. Its attenuation constant α is obtained by the following expression:

(3.4.9)

The phase and group velocities of the wave on the loaded dispersive line are

(3.4.10)

Figure (3.27b) shows the dispersion behavior, i.e. the function ω = f(β), on the (ω − β) diagram for the shunt inductor loaded line. It shows the frequency‐dependent behavior of the propagation constant β and attenuation constant α. The dashed line is the light line. Its slope ψ at the origin is the phase velocity of the EM‐wave in free space, i.e. v_p = v₀ = c. The propagation constant β exists above the light line only for ω > ω_c and wave attenuation occurs for ω < ω_c. At location P, the local slope ϕ provides the group velocity v_g, whereas the slope ψ of the point P at the origin O provides the phase velocity v_p of the propagating EM‐wave on the loaded transmission line.

Figure 3.27 Shunt inductor loaded line and its characteristics.

Figure (3.27c) shows the variations in the phase velocity and the group velocity with frequency. For ω → ω_c, v_p → ∞ , v_g → 0, and for ω → ∞, both wave velocities move toward the light line, i.e. toward the phase velocity (v₀) of the unloaded host transmission line. From equation (3.4.10a) dv_p/dω is negative, i.e. the phase velocity decreases with frequency, whereas from the equation (3.4.10b), dv_g/dω is positive, i.e. the group velocity increases with frequency. However, both velocities tend toward v₀, i.e. phase velocity in the unloaded host medium. Figure (3.27b) also shows that the propagation constant β increases with frequency. Thus, the shunt inductor loaded line has normal dispersion. The wave considered is a forward‐moving wave with both the phase and group velocities in the same direction, as both anti‐clockwise gradients ψ and ϕ defining the phase and group velocities respectively are positive. Above the cut‐off frequency, i.e. above the light line in the fast‐wave region, the phase velocity is higher than the phase velocity of the unloaded L‐C type transmission line. The shunt inductor loaded line supports the fast‐wave. The wave is fast as compared to the wave velocity, shown as the slope of the light line, on an unloaded transmission line.

The group velocity v_g is also frequency‐dependent, causing dispersion in the envelope of a wave‐packet. Therefore, if a voltage wave‐packet, say a Gaussian wave‐packet, propagates on a shunt inductor loaded line, it disperses while moving forward. Figure (3.27d) shows that its amplitude decreases and the pulse width increases. This is known as the group dispersion. The time delay of the envelope over the distance d is

(3.4.11)

In the present subsection, the propagation constant of the loaded line is obtained by solving the wave equation. However, the dispersion relation and also the characteristics impedance of the loaded line could be obtained from the circuit analysis. This simple method is applicable to several interesting cases of loaded lines forming the basis for the modern Electromagnetic bandgap (EBG) materials and metamaterials.