Simple T-line and its performance, S-Parameter Performance of a microstrip T-line, Design of uniform circular PBGSs for Harmonic Suppression, Standard BPF, BPF on 2-D array of uniform circular PBGSs, BPF with dense 2-D uniform circular PBGSs, BPF with PBGSs under 50-ohm and central coupled lines



    Simple T-line and its performance:
T-line is just a line with a defined length and width on the upper surface of the substrate which is created by removing copper coating from the surface except the desired region. The figure is shown below where the blue region is a typical T-line whose length is 100 mm and width is 2.2642 mm (calculated by PCAAD for 50Ω microstrip T-line where dielectric constant of the substrate is 2.45 and thickness is 31 mils).


Fig. 5.1: Geometry of a standard 50-ohm microstrip transmission line on a substrate whose dielectric constant is 2.45 and thickness is 31 mils.

S-Parameter Performance of a microstrip T-line:
S-Parameter performances are inspected from the plotted curves of the simulation by Zeland ie3d where the curves of S11 (return loss) and S21 (insertion loss) are only shown here. Stopband and passband yield the frequency band width of insertion loss and return loss at -20 dB and -10 dB respectively. The following graph is plotted by Grapher software by taking simulated data from the Zeland ie3d

Fig. 5.2: S-parameter performance of 50 Ω T-line whose length is 100 mm and width is
2.2642 mm.
Within the range of 0-20GHz the signal has transmitted between two ports with negligible
loss and there is no stopband formed. The return loss performance of the ideal microstrip
line over the whole frequency range is also excellent and < - 10 dB. Since, there is no
appreciable insertion loss observed at the s-parameter performance of the T-line, therefore
it characterizes an ideal transmission line.

        Design of uniform circular PBGSs for Harmonic Suppression


Uniform circular PBGSs are implemented to form different designs. PBG assisted BPF with different lattices and PBG elements have been investigated that include (i) BPF on 2-D array of uniform circular PBGSs which forms square lattice,  (ii) BPF on dense 2-D uniform circular PBGSs that forms rectangular lattice, (iii) BPF on 1-D uniform circular PBGSs that exactly located under the two extreme 50-ohm lines and the central coupled line, (iv) BPF on uniform circular PBGSs that are located under two extreme line only and finally (v) BPF on uniform circular PBGSs that are located under all the lines of a BPF. All these designs are shown in Fig. 6.20. These investigations are very useful to understand the behavior of poles of BPFs in the presence of PBGSs.

·         Standard BPF

A 4-section asymmetric coupled line BPF is shown in Fig. 6.20(a). The dimensions of the coupled lines are: W1 = 0.425 mm, W2 = 0.525 mm, G1 = 0.2 mm, G2 = 0.7 mm, L1 = L2 = 3.625 mm and W50 = 0.6 mm. The dimensions of the reference BPF are same as [32].

·         BPF on 2-D array of uniform circular PBGSs

In this design the uniform circular PBGSs are etched in the ground plane having their periodicities in X-and Y-directions that forms square patterned lattice structure. Here PBG elements form square lattice. The geometry is shown in Fig. 6.20 (b) that consists of 3 rows of 9 PBG elements.

·         BPF with dense 2-D uniform circular PBGSs

2-D array of uniform circular PBGSs are situated beneath all the lines of BPF including outside of the line having rectangular lattice structures. The Bragg’s condition is applied in X-direction. The geometry is shown in










·         BPF with PBGSs under 50-ohm and central coupled lines

Here PBG elements are located under 50-ohm and central coupled lines. This design consists of total 9 PBG elements. The geometry of this design is shown.

·         BPF with PBGSs under 50-ohm lines only

In this design, PBG elements are located under 50-ohm lines only. There are 6 PBG elements in this design as shown in .

·         BPF with uniform circular PBGSs under all lines only

Uniform circular PBGSs are under all the microstrip line of BPF thinking over the idea that the field is confined below the lines. Beyond the lines there are no PBG elements. The geometry is shown .

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