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Main characteristics of spiral
antennas are
• Circular polarization,
• Broad-band,
• Low directivity.
Models of duofilar spiral
antennas, simulated in WIPL-D Pro are presented here. One model
is made without the substrate (Fig. 1), while the other model is
a spiral printed on dielectric substrate (Fig. 2). Parameters of
the dielectric are:
•
,
•
.
Both models have a reflector.
Dimensions of metallic radiating
elements are the same in both models. Difference exists only in
added dielectric in the second model. Our aim is to investigate
the influence of the dielectric and to compare simulation times
and numbers of unknowns for these two models. We will observe
antennas’ gain starting from 1 GHz up to 5 GHz (D, E, F and G
bands–NATO band classification). |

Figure 1. Spiral antenna |
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WIPL-D Simulation
In WIPL-D Pro, helix antennas can be designed using the built-in
Helix object. Antenna shown in Fig. 1 can be also modeled
“manually” (using individual plates as building blocks) but that
would make modeling difficult. Frequency for calculation of
radiation pattern and near field is 3 GHz.
The 3D radiation pattern of the
spiral antenna without the dielectric is shown in Fig. 3.
Overlaid 2D radiation patterns for main direction are shown in
Fig. 4, for cases with and without the dielectric.
Near fields of the model immersed
with no dielectric is given in Fig. 5.
Number of unknowns, memory
requirements, and simulation time at a single frequency are
given in Tab. 1. Computer used for these calculations is Intel Core2 Quad CPU @ 2.83 GHz. |

Figure 2. Spiral antenna printed
on dielectric |
|

Figure 3. Radiation pattern of
spiral antenna without dielectric |

Figure 4. Overlaid gains for main
radiation direction |
|

Figure 5. Near field of spiral
antenna |
Table 1. Simulation data
|
Model |
No. of unknowns (memory [MB]) |
Time @ 3 GHz [sec] |
|
Air |
797 (5.1) |
<1 |
|
Dielectric |
5643 (254) |
13 |
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Conclusion
Using WIPL-D Pro Helix object with the possibilities for
parameterization, we can easily create and manipulate spiral antenna
structures. We can see that a great difference exists between gain of
antenna without dielectric and antenna printed on dielectric (Fig. 4).
Dielectric is necessary in antenna design in order to increase structure
solidity. Its presence shifts gain vs. frequency characteristic,
(changing maximal gain) and exact its electrical properties need to be
taken into account during the antenna design. Inclusion of the
dielectric significantly increases number of unknowns and simulation
time (Tab 1), but still the overall simulation performed in WIPL-D Pro
is very fast. Results given here by WIPL-D Pro coincide with theoretical
expectations.
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