Research Article  Open Access
Taimoor Khan, Asok De, "Estimation of Different Performance Parameters of Slotted Microstrip Antennas with AirGap Using Neural Networks", International Scholarly Research Notices, vol. 2014, Article ID 296105, 6 pages, 2014. https://doi.org/10.1155/2014/296105
Estimation of Different Performance Parameters of Slotted Microstrip Antennas with AirGap Using Neural Networks
Abstract
Over the past decade, artificial neural networks have emerged as fast computational medium for predicting different performance parameters of microstrip antennas due to their learning and generalization features. This paper illustrates a neural network model for instantly predicting the resonance frequencies, gains, directivities, antenna efficiencies, and radiation efficiencies for dualfrequency operation of slotted microstrip antennas with airgap. The proposed neural model is valid for any arbitrary slotdimensions and inserted airgap within their specified ranges. A prototype is fabricated using Roger’s substrate and its performance is measured for validation. A very good agreement is achieved in simulated, predicted, and measured results.
1. Introduction
There are many situations of wireless communication where dualfrequency operation is required such as satellite communication, radar systems, and global positioning system (GPS). Microstrip antennas (MSAs), because of operating in dualfrequency mode, have eliminated two singlefrequency operated antennas in these applications [1]. Different researchers have proposed different techniques for obtaining dual resonance such as multilayered stacked patch [2, 3], slotted rectangular patch [4], square patch with notches [5], patch loaded with shorting posts [6] or varactor diodes [7], and rectangular patch fed by an inclined slot [8]. These methods [2–8] can roughly be categorized as analytical methods and numerical methods. The analytical methods provide a good spontaneous explanation for the operation of MSAs. These techniques are based on the physical assumptions for simplifying the radiation mechanism of the MSAs but are not suitable for many microstrip structures where the thickness of the substrate is not very thin. On the other hand, the numerical methods provide accurate results but only at the cost of using complex mathematical expressions in the form of integral equations. The choice of test functions and path integrations appear to be more critical without initial assumptions in the final stage of the numerical results. Also, these approaches require a new solution even for an infinitesimal alteration in the geometry. Thus, the requirement for having a new solution for every small alteration in the geometry as well as the problems associated with the thickness of the substrates in analytical methods leads to complexities and processing cost [9]. Recently, artificial neural networks (ANNs) models have acquired tremendous applications in the wireless communication due to their ability and adaptability to learn and generalization features [9–16]. The ANN model is trained using measured, calculated or simulated patterns. The aim of the training process is to minimize error between reference and actual outputs of the ANN model. Once the model is trained for a specified error, it returns the results for every infinitesimal changes in the geometry both for electrically thin and thick MSAs within a fraction of a second. Several neural models are available in the literature [13–16] for computing single performance parameter (resonance frequency or geometric dimensions) of the microstrip patch antennas, respectively. But having individual neural model for each performance parameter becomes sometimes unattractive to include in modern antenna computeraideddesign (CAD) programs. It has recently been overcome by introducing the concept of generalized neural approach for computing different performance parameters, simultaneously [17–20]. The resonance frequencies of rectangular, circular, and triangular MSAs have been computed [17–19] using generalized neural networks model. The resonance frequencies and the physical dimensions of the rectangular MSAs have been computed using generalized neural networks model [20]. Hence, the individual neural models [9–16] and generalized neural approaches [17–20] have been used only for resonance frequency and/or geometric dimensions of microstrip patch antennas. Few neural networks models [21–23] have also been proposed for designing the slotted microstrip antennas. But unfortunately, simultaneous computations of different performance parameters (i.e., resonance frequency, gain, directivity, antenna efficiency, and radiation efficiency) using neural networks model have been rarely attempted in the available literature [9–23] as these parameters are essentially required for antenna designers for synthesizing the MSAs. In the proposed work, the authors have extended their earlier works of generalized neural networks modeling [24–30] for predicting different performance parameters (i.e., resonance frequencies, gains, directivities, antenna efficiencies, and radiation efficiencies) of slotted microstrip antennas for dualfrequency operation.
This paper is organized as follows. Proposed geometry of slotted microstrip antenna is discussed in Section 2. Section 3 describes proposed neural networks modeling. Experimental results and discussion are illustrated in Section 4. A conclusion followed by the references is discussed in Section 5.
2. Proposed Microstrip Antenna
The proposed geometry of slotted MSA is shown in Figure 1. A rectangular patch of dimensions 61 × 56 mm^{2} is designed with RTDuroid substrate RO3003 (, mm and ) using method of moment (MoM) based IE3D simulator [31]. Two resonating modes (TM_{10} and TM_{01}) are excited by a single probe for getting dual resonance. The performance of the patch antenna is further improved by inserting airgap of “” thickness between the substrate sheet and the ground plane [32]. A crossslot of dimensions, “x_{1},” “y_{1},” “x_{2},” and “y_{2}” is inserted on the radiating surface of rectangular patch microstrip antenna as shown in Figure 1. For each resonance, different performance parameters like gain, directivity, antenna efficiency, and radiation efficiency are observed by varying the slotdimensions (1 mm ≤ slotdimensions ≤ 50 mm) and inserted airgap (1 mm ≤ airgap ≤ 10 mm). Flexible analytical modeling for such a complicated situation is still a challenge in electromagnetic community [1]. To tackle such problems there is no way except using the neural networks for fast estimation of the performance parameters for each value of slotdimensions (1 mm ≤ slotdimensions ≤ 50 mm) and inserted airgap (1 mm ≤ airgap ≤ 10 mm) for the geometry shown in Figure 1. The artificial neural networks modeling for the proposed problem is discussed in Section 3.
(a) Top view
(b) Side view
3. Proposed Networks Modeling
In today’s highly integrated world, when solutions to problems are crossdisciplinary in nature, neural networks promise to become a powerful means for obtaining solutions to problems quickly and accurately. Artificial neural networks (ANNs) are massively distributed parallel processors that have natural propensity for storing experiential knowledge during training and making it available for use during testing. ANN models resemble the brain since knowledge is acquired by the network through a learning process, and interneuron connection strengths are used to store the knowledge [9]. Neural networks learn (or train) by known examples of a problem to acquire knowledge about it. Once the neural network is successfully trained, it can be put to effective use in solving “unknown” or “untrained” instances of the problem [9]. Multilayered perceptron (MLP) and radial basis function (RBF) neural networks have primarily been used in computing different performance parameters of the MSAs [9–30]. A radial basis function (RBF) neural network consists of threelayers feedforward neural networks in which each layer is having entirely different roles [18, 19]. As far as learning (or training) of the neural networks is concerned, the RBF neural networks are much faster than the MLP neural networks. It is so because the learning process in RBF neural networks has two stages and both the stages are made more efficient by using appropriate learning algorithms [28]. There are three common steps followed during training of a neural networks model. Firstly, the training patterns are generated, then the structural configuration of hidden layer neurons is selected in the second step and finally, in the third step the weights are optimized by using training algorithm. For the first step, total 1350 patterns (1000training + 350testing patterns) are generated by varying the slot dimensions (1 mm ≤ x_{1}, y_{1}, x_{2}, y_{2} ≤ 50 mm) and airgap (1 mm ≤ ≤ 10 mm) for the geometry shown in Figure 1. The structural configuration and training strategy of the proposed neural model are being discussed here.
To build a neuralnetworkbased application, training stage is one of the more critical phases of the neural networks. Methods created from the field of optimization theory have played an important role in developing training algorithms for neural networks. Training a neural network model basically consists of adjusting weights with the help of a training algorithm. Before doing training, the generated patterns are normalized between +0.1 and +0.9 using MATLAB software [33]. The training performance of the proposed neural model is observed by varying the number of neurons in the hidden layer and after many trials, it is optimized with forty nine neurons for the best performance. Further, the training performance of the model is observed with seven different training algorithms, respectively [33–35]. These are mentioned as BFGS quasiNewton (BFG), Bayesian regulation (BR), scaled conjugategradient (SCG), PowellBeale conjugate gradient (CGB), conjugate gradient with FletcherPeeves (CGF), one step secant (OSS), and LevenbergMarquardt (LM).
A RBF neural network model for computing different performance parameters is illustrated in Figure 2 in which input layer is having sixdimensional excitation matrix and output layer twodimensional response matrix . Here variables “x_{1},” “y_{1},” “x_{2},” and “y_{2}” represent the dimensions of the crossslot and “t” indicates the inserted airgap between the ground plane and the substrate (see Figure 1). As a common neural network model is being created for predicting different performance parameters of slotted MSAs for each value of slotdimension and inserted airgap, hence it becomes necessary to distinguish these performance parameters. For this purpose, an arbitrary parameter “M” is included in the input patterns during training of the neural model. The parameter, “M,” is treated here as mode control where M = 1, 2, 3, 4, and 5 corresponds to dualresonance (DR), dualfrequency gains (DFG), dualfrequency directivities (DFD), dualfrequencies antenna efficiencies (DFA), and dualfrequencies radiation efficiency (DFR), respectively. Thus sixdimensional input pattern and twodimensional output pattern are used during training as well as testing of the proposed RBF neural networks model. The block diagram used for training the proposed neural networks model is shown in Figure 2(a) whereas computations of different performance parameters during testing of the neural model are shown in Figures 2(b)–2(f).
(a)
(b)
(c)
(d)
(e)
(f)
The structural configuration for the proposed RBF neural model shown in Figure 2(a) is mentioned as . For an applied input pattern, some random values between 0 and 1 are assigned to the weights and the output of the model is computed corresponding to that input pattern. The mean square error (MSE) between calculated and simulated results is then computed and all the weights are updated accordingly using a training algorithm. In the proposed neural modeling scheme seven different training algorithms, BFG, BR, SCG, CGB, CGF, OSS, and LM, are used [33–35]. This updating process is carried out after presenting each set of input pattern until the calculated accuracy of the neural model is deemed satisfactory. This updating process is completed by considering the training parameters: , learning rate , momentum coefficient , spread value , dimensionality of input pattern , dimensionality of output pattern , total number of pattern , number of training patterns , and number of testing pattern . After optimizing the weights, the testing algorithm is implemented for the remaining 350 samples which were not included in 1000 training samples of the RBF model. For this implementation the initial weights are replaced by the optimized weights. The trained neural model now returns the response within a fraction of a second for any arbitrary values of crossslot dimensions (1 mm ≤ slotdimensions ≤ 50 mm) and airgap (1 mm ≤ airgap ≤ 10 mm). Computations of different performance parameters during testing of the neural model are illustrated in Figures 2(a)–2(f).
4. Experimental Validation
The neural networks modeling scheme is discussed in Section 2 for instantly predicting the desired performance parameters of the slotted microstrip antennas with inserted airgap for dualfrequency operation. The training performance of the proposed neural model is observed with seven different algorithms, BFG, BR, SCG, CGB, CGF, OSS, and LM, respectively. In the present work, only LevenbergMarquardt (LM) backpropagation is proved to be the fastest converging training algorithm as it requires only 1489 sec. for training which is lower than that of other training algorithms. Further, for the proposed problem, this algorithm is also observed as more accurate than that of other algorithms.
The trained neural model returns the response for every infinitesimal change in the slotdimension and airgap within their specified ranges. It is tested for 350 samples of slotdimension and airgap. The percentage error in computing the performance parameters for the first resonance (TM_{10} mode) is calculated. Thus, the average discrepancies between simulated and predicted values are observed as 1.92%, 0.9992%, 1.0937%, 2.9007%, and 2.9490% in resonance frequencies, gains, directivities, antenna efficiencies, and radiation efficiencies, respectively. A graph is plotted in Figure 3 only for 50 values corresponding to first resonance (TM_{10} mode). It is clear from Figure 3 that most of the predicted outcomes are in very good agreement with their simulated counterparts and only few are far off.
For validating the proposed work, a prototype is fabricated using RTDuroid substrate RO3003 ( and mm). The patch of dimensions 61 mm × 56 mm is etched on upper side of the substrate whereas an airgap of 5.1 mm is stacked using Teflon rods between substrate and ground plane of dimensions 200 × 175 mm^{2}. The Sparameters of the fabricated prototype are measured using Agilent N5230A network analyzer and the setup used for this measurement is shown in Figure 4. The prototype is excited by probe feed which guides the electromagnetic waves to the feed point. The energy of electromagnetic waves then spreads out into the region under the slotted patch, some of which cross the boundary of the slotted patch and radiate into the halfspace above the patch. An SMA connector with 6.8 mm long pin (1 mm for ground plane + 5.1 mm for airgap + 0.762 mm for substrate) is used for RF connection between the ground plane and the slotted patch. Table 1 shows the measured results of the fabricated prototype. A good convergence among the simulated, calculated, and measured results confirms that the Taflon rods do not affect the antenna performance.

The performance parameters of the original geometry (without crossslot) and crossslotted geometry are studied and an improvement by inserting the crossslot in the fabricated prototype is summarized in Table 2. In the fabricated prototype, by inserting a crossslot, the excited surface current path lengthens, increasing the antenna length and hence decreasing the resonance frequency. For the case of slotted patch, both the resonance frequencies (1.763 GHz and 1.914 GHz) are lowered by ~13% as compared to those (2.0256 GHz and 2.1970 GHz) of the simple rectangular patch without a crossslot. This reduction in the frequencies can result in a patch size reduction of ~35% for a given dualfrequency design. Hence a good rank of compactness is achieved in the fabricated prototype. Also, the ratio of two frequencies (1.914/1.763 = 1.0857 and 2.1970/2.0256 = 1.0846) is slightly affected by inserting the crossslot and mainly determined by the aspect ratio (1.89 = 61/56) of the patch, which makes the design simpler and easier to implement.

During simulation a bandwidth of 55.5 MHz is achieved but it increases to 250 MHz (1.99 GHz–1.74 GHz) in fabricated prototype during measurement for S_{11} ≤ −10 dB (see Figure 4). It may be probably due to irregularity in fabricating the prototype and/or inserting the airgap by using the Teflon rods. Further in the simulation, we do not consider the size and loss of the solder joint, which may cause this difference between the measured and simulated bandwidth. A very good impedance matching is also achieved by inserting an airgap of 5.1 mm (see Figure 4). The efficiencies (both antenna and radiation efficiencies) are improved because of negligible amount of dielectric loss in the airlayer. As gain of an antenna is defined as the product of directivity and radiation efficiency, hence the gain is also improved.
5. Conclusion
In this paper, a fast and accurate neural networks approach has been proposed for predicting different performance parameters of slotted microstrip antennas for dualresonance. Using this approach, various radiation characteristics of the microstrip antennas for arbitrary slotdimensions and airgap within their specified ranges have been computed. The proposed approach is capable of computing ten different parameters (dualresonance, dualfrequency gains, dualfrequency directivities, dualfrequency antenna efficiencies, and dualfrequency radiation efficiencies), simultaneously as such an approach is rarely proposed in the literature for the best of our knowledge.
For validation a prototype has been fabricated and an airgap has been stacked using Taflon rods between the ground plane and the substrate sheet. The performance of the fabricated prototype has been characterized using Agilent N5230A network analyzer. A very good convergence in the measured, calculated, and simulated results has been achieved.
In general, the neural model for computing ten different parameters may require ten different modules, whereas in the present work, only one model is fulfilling the requirement of the ten modules. Hence, this approach can be considered more generalized. This approach is simple and accurate that it can further be extended to a large number of computing parameters depending upon the required accuracy and structural configuration of the neural networks. Because of simplicity one can calculate the desired performance parameters for the given arbitrary values of slotdimensions and airgap within their specified ranges using a personal computer (PC) without having the fundamental knowledge of microstrip antennas. It takes only a fraction of a second in producing the required result on a computer system after being trained properly. As the approach has produced more accurate results in computing ten different parameters, hence it can be recommended to include in antenna computeraideddesign (CAD) algorithms.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
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Copyright
Copyright © 2014 Taimoor Khan and Asok De. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.