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Dual Band Antennas For Sale

Progress In Electromagnetics Research C, Vol. 9, 171–182, 2009
COMPACT SHORTED MICROSTRIP PATCH ANTENNA FOR DUAL BAND OPERATION A. Mishra, P. Singh, N. P. Yadav, and J. A. Ansari Department of Electronics & Communication University of Allahabad Allahabad 211002, India B. R. Vishvakarma Department of Electronics Engineering I. T. BHU Varanasi 221005, India Abstract—In the present paper notch loaded shorted microstrip patch antenna has been analysed using cavity model. The proposed antenna shows dual band operation which depends on notch dimensions as well as shorting wall. The frequency ratio is found to be 1.5278 for the notch loaded rectangular patch, while in notch loaded shorted patch, the frequency ratio varies from 2.9764 to 2.725 for increasing value of notch width and it is almost invariant with notch depth. Further a slot loaded shorted patch antenna shows the dual frequency nature with the frequency ratio 1.7. The theoretical results are compared with IE3D simulation as well as reported experimental results. 1. INTRODUCTION Compact microstrip antennas have received much attention due to increasing application of small antennas for personal communication equipments [1–5]. Shorted patch antennas have been reported to overcome the size constraints for a variety of communication link. Recently it has been demonstrated that loading the microstrip antenna with shorting pin and shorted wall can reduce the patch size for a fixed operating frequency [6–9]. Various kind of microstrip antennas have been proposed to achieve dual band operation such as redial slot [10], microstrip patch antenna Corresponding author: A. Mishra ([email protected]).
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with π shaped slot [11]. One of the most popular techniques to obtain the dual band frequency is reactive loading by introducing the slots parallel to radiating edge of the patch [12] and cutting square slot in the patch [13, 14]. Another type of reactive loading can be introduced to get higher frequency by cutting a notch parallel to the rediating edge of the patch [15]. In this paper, two antenna geometries are analysed for dual band operation using the circuit theory concept. In first geometry, a notch with dimension (Ln × Wn ) is introduced along one of the radiating edge and another radiating edge is shorted with shorting wall, while in second geometry, a slot with dimension (Ls × Ws ) is loaded in rectangular microstrip patch antenna with shorted wall. Various antenna parameters are calculated as a function of frequency for different values of notch and slot dimensions. 2.1. Analysis of Notch Loaded Shorted Patch Antenna The geometry of proposed antenna is shown in Fig. 1. A simple rectangular microstrip patch antenna can be analysed as a parallel combination of R1 , L1 and C1 as shown in Fig. 2, where R1 , L1 and C1 can be defined as [16]. εe εo LW cos−2 (πxo /L) 2h 1 L1 = 2 ω C1 Qr R1 = ωC1 C1 =
(1) (2) (3)
Y
L
h
shorting wall
Ln Wn
X W
R1
L1
C1
S Z
feed point
Figure 1. Geometry of notch loaded shorted patch antenna.
Figure 2. Equivalent circuit of rectangular patch.
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in which L = length of the rectangular patch W = width of the rectangular patch xo = feed point location along length of the patch h = thickness of the substrate material and
√ c εe Qr = fh
where c = velocity of light f = design frequency εe = effective permittivity of the medium which is given by [16] ¡ ¢−1/2 εe = εr2+1 + εr2−1 1 + 10h W where, εr = relative permittivity of the substrate material. The notch is introduced along one of the radiating side and other side is shorted by the shorting wall. Due to the effect of notch, the two current flows in the patch, one is the normal patch current and resonates at the design frequency of the initial patch; however, the other current flows around the notch consequently alters the resonance frequency, as shown in Fig. 3. Due to this discontinuity an additional series inductance (∆L) and series capacitance (∆C) appear that modify the equivalent circuit of
(a)
(b)
Figure 3. Current distributions of notch loaded shorted patch antenna: (a) f r1 = 2.731 GHz, (b) f r2 = 8.01 GHz.
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RMSA as shown in Fig. 4, in which series inductance (∆L) and series capacitance (∆C) can be calculated as [17, 18]. hµ0 π ∆L = (Ln /L)2 8 and ∆C = ( LLn ) · CS where µ0 = 4π × 10−7 H/m Ln = depth of the notch Cs = gap capacitance and is given by [19]. It may be noted that the two resonant circuits, one is the initial R L C of the shorted patch shown in Fig. 5 and another one is after cutting the notch, are coupled through mutual inductance (Lm ) and mutual conductance (Cm ). Now the equivalent circuit of the proposed antenna can be given as shown in Fig. 6. The input impedance of the notch loaded microstrip patch can be calculated as Zshort Zm ZT = Znotch + (4) Zshort + Zm where Zshort = input impedance of the shorted patch and can be given as R1 jω Zshort = (5) jω + LT R1 − R1 C1 ω 2 in which LS + L1 LT = L1 LS where LS = Inductance due to shorting wall and defined as [16] ¸ · (S + t) 2h + 0.2235 + 0.5 LS = 0.2h log (S + t) h
L1
C1
Ls R1
L1
C1
R1 ∆C
Rs
Figure 4. Equivalent circuit of patch due to effect of notch.
Figure 5. Equivalent circuit of shorted patch antenna.
∆L
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where S = length of the shorting wall h = height of the substrate i.e., width of the shorting wall t = thickness of the shorting wall Znotch =
jωR1 L2 jωL2 + R1 − R1 L2 C2 ω 2
(6)
where L2 = L1 + ∆L C1 ∆C C2 = C1 + ∆C and Zm
µ = jωLm +
1 jωCm
¶
where Lm and Cm are the mutual inductance and mutual capacitance between two resonant circuits and given as [20]. q Cp2 (L1 + L2 ) + Cp2 (L1 + L2 )2 + 4Cp2 (1 − Cp2 )L1 L2 Lm = (7) 2(1 − Cp2 ) q (C1 + C2 ) + (C1 + C2 )2 − 4C1 C2 (1 − Cp−2 ) Cm = − (8) 2 where Cp = √Q1 Q and Q1 and Q2 are quality factors of the two 1 2 resonant circuits. Z notch
Z shorted
Y L
shorting wall
Lm W
LS
X S
Cm Z
Figure 6. Equivalent circuit of coupled notch loaded shorted patch antenna.
WS
feed point
Figure 7. Geometry of slot loaded shorted patch antenna.
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2.2. Analysis of Slot Loaded Shorted Patch Antenna The geometry of slot loaded shorted patch antenna is shown in Fig. 7. The slot on the patch can be analysed by using the duality relationship between the dipole and slot [21]. The corresponding current distribution for the slot loaded shorted patch is shown in Fig. 8. The input impedance of a single slot parallel to the radiating edge can be given as [22]. ¶ Z µ −jkr1 e e−jkr1 e−jkr0 ZS = j30 + − 2 cos kh sin k(h − |z|)dz (9) r1 r2 r0 where k = 2π/λ, λ thickness of the substrate
=
wavelength in the medium,
h
=
£ ¤1/2 r1 = y 2 + (h + z)2 £ ¤1/2 r2 = y 2 + (h − z)2 £ ¤1/2 r0 = y 2 + z 2
Equation (9) can be given as ZS = Rslot + jXS
(10)
where RS is the real part of the Eq. (10) and equivalent to radiation resistance of the slot and imaginary parts XS is input reactance of the
(a)
(b)
Figure 8. Current distributions of slot loaded shorted patch antenna: (a) f r1 = 2.4 GHz, (b) f r2 = 4.1 GHz.
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Dual Band Slot Loaded Patch Antenna