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Reconfigurable Microstrip Antenna with Two- Dimensional Scannable Beam Ahmed Khidre (1) , FanYang (1,2) , and Atef Z. Elsherbeni (1) (1) Center of Applied Electromagnetic Systems Research, Electrical Engineering Department, The University of Mississippi University, MS 38677, USA (2) Microwave and Antenna Institute, Electronic Engineering Department, Tsinghua University Beijing 100084, P. R. China [email protected], [email protected], [email protected] Abstract—This paper proposes a reconfigurable microstrip antenna with two-dimensional beam scanning feature. The antenna geometry consists of two parasitic patches placed along the E and H-planes of a probe-fed patch. Each parasitic patch is loaded with a lumped varactor and DC biasing network, to effectively change its electrical size. Because the main beam direction is determined by the electrical size of the parasitic patches, electronic beam scanning is allowed by changing the capacitance value through the applied DC voltage. Consequently, Two DC control signals are used for the two-dimensional beam scanning. Operating at 2.5 GHz, the antenna shows a beam scanning that ranges from 0 to 32 in the elevation plane and from 0 to 90 in the azimuth plane. The attained peak gain value is 8.51 dBi with 0.8 dB gain variation across the entire scanning range. I. INTRODUCTION The recent demand of compact wireless devices propels the development of pattern reconfigurable antennas. They can steer their beam direction that helps in avoiding noisy environment, and strengthening the signal detection from an intended target. Classically, beam steering is realized with phased arrays, but it might be too large or complex to meet the demand of compactness or cost reduction. In [1], Yagi-Uda based microstrip antenna with a pattern reconfigurable feature is proposed. However, they allow for beam switching to fixed directions, rather than continuous beam scanning. In [2], continuous beam scanning is achieved by loading the antenna with variable reactive elements. However, the radiation beam is allowed to be only scanned in one plane (one-dimensional). In this paper, a reconfigurable microstrip antenna with a continuous two-dimensional (2D) beam scanning feature is proposed. The antenna geometry consists of two square parasitic patches, placed along the E and H-planes of a square probe-fed patch. A varactor diode with a proper DC biasing network is added to each parasitic patch, to effectively change its electrical size. Because the main beam direction is determined by the electrical size of the parasitic patches [3], [4], electronic beam scanning is achieved by changing the applied DC voltage (capacitance value). Two DC control signals are required to scan the beam in two dimensions. The antenna design is performed using a full wave simulation for 2.5 GHz operating frequency. II. OPERATIONAL PRINCIPLES When a parasitic patch is placed along the E or H plane of a driven patch at a certain separation distance, the total radiation beam tilts away from the bore sight direction in that plane, due to the existing coupling between them [3]. Basically, if the parasitic patch is smaller than or equal to the driven one, it acts as a director and the beam tilts toward the direction of its side. The main beam tilt angle is determined by the size of the parasitic patch, and the maximum tilt angle occurs when the parasitic patch size is close to the driven one as illustrated in [4]. Also, if the parasitic patch is too small, the coupling become weak and loses its effect, therefore the main beam shifts towards the broadside direction. The antenna geometry, shown in Fig. 1, consists of three square patches. One is fed with a probe and its dimensions are 38 x 38 mm. The other two are parasitic and are placed to the top and right of the driven patch. The dimensions in mm of the geometrical parameters L r1 x L r1 and L r2 x L r2 are listed in Table I. The substrate has thickness h=3.175 mm, and relative permittivity r =2.2. The ground plane size is 150 x 150 mm. We have found that, when the size of the top parasitic patch is very small (L r1 =25mm), and right parasitic patch size is close to the driven patch size (L r1 ~37mm), the beam is directed toward the positive x axis with an elevation angle θ m =32 ° (Case A). Upon the gradual enlargement of the top patch, the beam is scanned in the azimuth plane along the clockwise direction, with a similar elevation angle. When the top patch size becomes equal to the right one, m =45 ° (Case B). If the right patch size is gradually reduced beyond this point, the beam continues to be scanned with a similar elevation angle in the azimuth plane, clockwise direction. When its size becomes too small to be effective, case C is reached. Case C is the reverse of Case A, at which the beam is directed toward the positive y axis instead. If the elevation angle is required to be reduced, the maximum value of the parasitic patches dimensions should be reduced further relative to the driven patch size. Table I summarizes the beam directions at different dimensions of the parasitic patches. The above elaborated phenomenon is the principle of the azimuthal beam scanning in the top right quadrant. Indeed, if a tuning mechanism is introduced to the sizes of the parasitic patches, electronic azimuthal beam scanning would be allowed. 196 978-1-4673-5317-5/13/$31.00 ©2013 IEEE AP-S 2013
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Page 1: Reconfigurable Microstrip Antenna with Two-Dimensional ...inside.mines.edu/...reconfigurable_microstrip_with_2D_scannable_be… · Abstract This paper proposes a reconfigurable microstrip

Reconfigurable Microstrip Antenna with Two-Dimensional Scannable Beam

Ahmed Khidre(1), FanYang(1,2), and Atef Z. Elsherbeni(1)

(1)Center of Applied Electromagnetic Systems Research, Electrical Engineering Department,

The University of Mississippi University, MS 38677, USA

(2)Microwave and Antenna Institute, Electronic Engineering Department,

Tsinghua University Beijing 100084, P. R. China

[email protected], [email protected], [email protected] Abstract—This paper proposes a reconfigurable microstrip antenna with two-dimensional beam scanning feature. The antenna geometry consists of two parasitic patches placed along the E and H-planes of a probe-fed patch. Each parasitic patch is loaded with a lumped varactor and DC biasing network, to effectively change its electrical size. Because the main beam direction is determined by the electrical size of the parasitic patches, electronic beam scanning is allowed by changing the capacitance value through the applied DC voltage. Consequently, Two DC control signals are used for the two-dimensional beam scanning. Operating at 2.5 GHz, the antenna shows a beam scanning that ranges from 0� to 32� in the elevation plane and from 0� to 90� in the azimuth plane. The attained peak gain value is 8.51 dBi with 0.8 dB gain variation across the entire scanning range.

I. INTRODUCTION The recent demand of compact wireless devices propels the

development of pattern reconfigurable antennas. They can steer their beam direction that helps in avoiding noisy environment, and strengthening the signal detection from an intended target. Classically, beam steering is realized with phased arrays, but it might be too large or complex to meet the demand of compactness or cost reduction. In [1], Yagi-Uda based microstrip antenna with a pattern reconfigurable feature is proposed. However, they allow for beam switching to fixed directions, rather than continuous beam scanning. In [2], continuous beam scanning is achieved by loading the antenna with variable reactive elements. However, the radiation beam is allowed to be only scanned in one plane (one-dimensional).

In this paper, a reconfigurable microstrip antenna with a continuous two-dimensional (2D) beam scanning feature is proposed. The antenna geometry consists of two square parasitic patches, placed along the E and H-planes of a square probe-fed patch. A varactor diode with a proper DC biasing network is added to each parasitic patch, to effectively change its electrical size. Because the main beam direction is determined by the electrical size of the parasitic patches [3], [4], electronic beam scanning is achieved by changing the applied DC voltage (capacitance value). Two DC control signals are required to scan the beam in two dimensions. The antenna design is performed using a full wave simulation for 2.5 GHz operating frequency.

II. OPERATIONAL PRINCIPLES When a parasitic patch is placed along the E or H plane of a

driven patch at a certain separation distance, the total radiation beam tilts away from the bore sight direction in that plane, due to the existing coupling between them [3]. Basically, if the parasitic patch is smaller than or equal to the driven one, it acts as a director and the beam tilts toward the direction of its side. The main beam tilt angle is determined by the size of the parasitic patch, and the maximum tilt angle occurs when the parasitic patch size is close to the driven one as illustrated in [4]. Also, if the parasitic patch is too small, the coupling become weak and loses its effect, therefore the main beam shifts towards the broadside direction. The antenna geometry, shown in Fig. 1, consists of three square patches. One is fed with a probe and its dimensions are 38 x 38 mm. The other two are parasitic and are placed to the top and right of the driven patch. The dimensions in mm of the geometrical parameters Lr1 x Lr1 and Lr2 x Lr2 are listed in Table I. The substrate has thickness h=3.175 mm, and relative permittivity �r=2.2. The ground plane size is 150 x 150 mm.

We have found that, when the size of the top parasitic patch is very small (Lr1=25mm), and right parasitic patch size is close to the driven patch size (Lr1~37mm), the beam is directed toward the positive x axis with an elevation angle θm=32° (Case A). Upon the gradual enlargement of the top patch, the beam is scanned in the azimuth plane along the clockwise direction, with a similar elevation angle. When the top patch size becomes equal to the right one, �m=45° (Case B). If the right patch size is gradually reduced beyond this point, the beam continues to be scanned with a similar elevation angle in the azimuth plane, clockwise direction. When its size becomes too small to be effective, case C is reached. Case C is the reverse of Case A, at which the beam is directed toward the positive y axis instead. If the elevation angle is required to be reduced, the maximum value of the parasitic patches dimensions should be reduced further relative to the driven patch size. Table I summarizes the beam directions at different dimensions of the parasitic patches. The above elaborated phenomenon is the principle of the azimuthal beam scanning in the top right quadrant. Indeed, if a tuning mechanism is introduced to the sizes of the parasitic patches, electronic azimuthal beam scanning would be allowed.

196978-1-4673-5317-5/13/$31.00 ©2013 IEEE AP-S 2013

Page 2: Reconfigurable Microstrip Antenna with Two-Dimensional ...inside.mines.edu/...reconfigurable_microstrip_with_2D_scannable_be… · Abstract This paper proposes a reconfigurable microstrip

(a) (b) (c)

Figure 1. Mictorstrip patch antenna with two parastic patches placed along the xz (E) and yz (H) planes: (a) case A; (b) case B; (C) case C.

Table I. Beam direction vs. parastic patch dimensions at 2.5 GHz

Top patch Lr1

(mm) Right patch Lr2

(mm) Direction (θm

°, �m°)

(degrees)

Case A 37 25 32°, 0° 36 25 25°, 0°

Case B 37 37 32°, 45° 36 36 25°,45°

Case C 25 37 32°, 90° 25 36 25°, 90°

(a) (b)

Figure 2. The proposed reconfigurable antenna for 2-dimensional beam scanning along with the baising assemblies: (a) geometry; (b) schematic for the beam direction trajoctry.

III. ANTENNA DESIGN AND PERFORMANCE A patch antenna with a capacitor loaded slot proposed in

[5], effectively provides the fundamental mechanism for tuning its electrical size. The relation between the capacitance values C versus electrical size Lr is discussed in [4]. Therefore, the parasitic patches in Fig. 1 are replaced with such antenna, and the proposed reconfigurable antenna for 2D beam scanning is constructed as shown in Fig. 2a. The dimensions of all the patches are 38 x 38 mm, whereas the slot of each parasitic patch is 20 x 0.5 mm. Two varactor diodes of capacitances C1 and C2 are placed in each slot along with the biasing circuits. Each parasitic patch is divided into two parts at its center by narrow slits of 0.2 mm width. The right part is fed with the DC signal through a metallic pin and a RF choke coil for RF/DC isolation. The left part is grounded through a shorted λ/4 transmission line.

The combinational change in the applied biasing voltage (capacitance value) to each parasitic patch, allows for the tuning of their electrical size simultaneously, hence electronic beam scanning would be enabled as shown in Fig. 2b. The simulation results for the radiation patterns at different combinations of C1 and C2 are shown in Figs. 3 and 4. As can be seen, the beam is rotating from �m=0° to 90° with θm~32°. Across the tuning range, the attained peak gain value is 8.5 dBi with 0.8 dB variation, whereas the maximum side lobe level is

-2.8 dB. Also, the x-polarization level within the beam width of the major beam is < -10 dB. In a similar fashion, full azimuthal beam scanning could be allowed if two more parastic patches with two varactors and their biasing assemblies are placed to the left and bottom of the driven patch.

u

v

-1 -0.5 0 0.5 1

-1

-0.5

0

0.5

1 -20

-15

-10

-5

u

v

-1 -0.5 0 0.5 1

-1

-0.5

0

0.5

1 -20

-15

-10

-5

u

v

-1 -0.5 0 0.5 1

-1

-0.5

0

0.5

1 -20

-15

-10

-5

(a) (b) (c)

Figure 3. The projected 3D radition pattern at different values of C1 and C2 : (a) C1=1.6, C2=2.5 pF; (b) C1=2.5, C2=2.5 pF; (c) C1=2.5, C2=1.6 pF.

-90 -60 -30 0 30 60 90-25-20-15-10

-505

10

θ(o)

RG

(dB

i)

co-polx-pol

φ=0o

-90 -60 -30 0 30 60 90-25-20-15-10

-505

10

θ(o)

RG

(dB

i)

co-polx-polφ=45o

-90 -60 -30 0 30 60 90

-25

-20

-15

-10

-5

0

5

10

θ(o)

RG

(dB

i)

co-polx-polφ=90o

(a) (b) (c)

Figure 4. The raition patterns in plane cuts of maximum radiation: (a) C1=1.6, C2=2.5 pF; (b) C1=2.5, C2=2.5 pF; (c) C1=2.5, C2=1.6 pF.

IV. CONCLUSION A new design of a reconfigurable microstrip antenna with

continuous 2-dimensional beam scanning patch has been proposed, using tunable size parasitic patches method. Electronic beam scanning is attained with the aid of varactors and proper biasing network integrated into the parasitic patch. The achieved scanning range is from 0� to 32�, 0° to 90° in the elevation and azimuth planes, respectively. The peak gain value is 8.5 dBi with less than 1 dB variation across the entire scanning range. Vehicular satellite receiving system is one of the potential applications for the proposed antenna.

ACKNOWLEDGEMENT This work was supported by NASA EPSCoR program under the contract number NNX09AP18A.

REFERENCES [1] X. Yang, B. Wang, S. Yeung, Q. Xue, and K. Man, “Circularly

Paolrized Reconifgurable Crossed-Yagi Patch Antenna,” IEEE Ant.Propag. Mag., vol. 53, no. 5, pp. 65-80, October 2011.

[2] L. Zhang, F. Yang, and A. Z. Elsherbeni, “ Analysis and Design of a Reconfigurable Dual-Strip Scanning Antenna,” in IEEE AP-S Int. Antenna and Propag. Symp. Digest, 2009.

[3] J. Huang and A. C. Densmore, “Microstrip Yagi array antenna for mobile satellite vehicle application,” IEEE Trans. Ant. Propag., vol. 39, no. 7, pp. 1024–1030, 1991.

[4] A. Khidre, F. Yang, and A. Z. Elsherbeni, “Reconfigurable Microstrip Yagi-Uda Antenna with a Scannable Circularly Polarized Beam,” in IEEE AP-S Int. Antenna and Propag. Symp. Digest, July 2012.

[5] A. Khidre, F. Yang, and A. Z. Elsherbeni, “Reconfigurable Dual-Band Patch Antenna with a Varactor-Loaded Slot,” in IEEE AP-S Int. Antenna and Propag. Symp. Digest, July 2012.

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