Modified Wilkinson Power Divider Using Transmission Lines for Various Terminated Impedances and an Arbitrary Power Ratio

Article information

J. Electromagn. Eng. Sci. 2019;19(1):42-47

Publication date (electronic) : 2019 January 31

doi : https://doi.org/10.26866/jees.2019.19.1.42

Young-Chul Yoon ¹, Young Kim ²^,

¹Department of Electronics Engineering, Catholic Kwandong University, Gangneung, Korea

²School of Electronics Engineering, Kumoh National Institute of Technology, Gumi, Korea

^*Corresponding Author: Young Kim (e-mail: youngk@kumoh.ac.kr)

Received 2018 July 10; Revised 2018 October 3; Accepted 2018 October 30.

Abstract

This paper introduces a modified Wilkinson power divider that uses uniform transmission lines for various terminated impedances and an arbitrary power ratio. For the designed power ratio, the proposed divider changes only the electrical lengths of the transmission lines between the input and output ports, and those between the output ports and the isolation resistor. In this case, even when various termination impedances of the ports exist, the divider characteristics are satisfied. To verify the feasibility of the proposed divider, two circuits were designed to operate at a frequency of 2 GHz with 2:1 and 4:1 power splitting ratios and various terminated impedances of 40, 70, and 60 Ω for one circuit, and 50, 70, and 60 Ω for the other. The measurement and simulation results were in good agreement.

Keywords: Arbitrary Power Ratio; Unequal Divider; Uniform Transmission Line; Various Terminated Impedance; Wilkinson Divider

I. Introduction

The divider is the most widely used passive component in the wireless industry. In many cases, the same splitting divider is used [1, 2]. However, in special applications, cases that require unequal distribution [3, 4] or various termination impedances [5, 6] exist. To achieve a divider with unequal or various terminated impedances, a high-impedance transmission line must be implemented. Such a high-impedance transmission line is difficult to implement because of its very narrow line width that must be implemented through microstrip technology. Moreover, to satisfy the characteristics of the high-impedance line, a bulky capacitor or coupled lines with narrow gaps are used.

Recently, a new design method has been proposed to adjust only the electrical length of the transmission lines between the input and output ports, or between the output ports and the isolation resistor, to achieve the operation of an unequal divider. Many dividers using a uniform transmission line have been introduced, such as a divider with uniform transmission lines of various electrical lengths [7–9], a structure using an isolated resistor with open-stub connection to obtain enhanced bandwidth [10], an isolated resistor configuration connected to the same impedance lines between the output ports with long stub length [11], a structure connected to various impedance lines at both sides of an isolation resistor [12], a Gysel divider with a phase shifter instead of a 180° transmission line [13], a ring hybrid coupler with a 50-Ω transmission line [14], and a half mode substrate integrated waveguide (HMSIW) divider with composite right and left-handed transmission line (CRLH-TL) [15]. This type of splitter uses a transmission line with uniform impedance, and it does not use an impedance transformer to match each port, even though it operates as an unequal divider. Such a divider consists of circuits with an arbitrary power split ratio and a termination impedance of 50 Ω.

In this paper, we propose a modified Wilkinson divider using a uniform transmission line with various termination impedances and an arbitrary dividing ratio as well as the previously used 50 Ω termination impedance. This type of device eliminates the requirement for a matching circuit between the divider and the peripheral device with various termination impedances, and allows a small circuit size to be achieved.

II. Theory and Design

Fig. 1 shows the schematic of the proposed power divider with power splitting ratio k² (= P₂/P₃). This proposed divider consists of three transmission lines with uniform impedance Z_uL and various electrical lengths of θ₁_L, θ₂_L, and θ₃_L, an isolation resistor R_iso, and various terminated impedances of R_aT, R_bT, and R_cT.

Fig. 1

Schematic of the proposed Wilkinson power divider.

In addition, this divider must satisfy the S-parameter characteristics of the unequal Wilkinson power divider:

(1) (S)unequal=11+k2(0k·e-jβe-jβk·e-jβ00e-jβ00)

where β is the phase shift of the transmission coefficient.

Because the proposed power divider with various terminated impedances is asymmetrical, we analyzed it using scattering parameters rather than the conventional even-odd method. When port 1 is excited, all power is transmitted to the output ports, P₂ and P₃, and the voltage from the branch of P₁ – P₂ to ground is the same as that from the branch of P₁ – P₃ to ground at any distance from P₁, and no current flows in the isolation resistor. Because the isolation resistor operates as an open circuit, we can design an equivalent circuit between ports 2 and 3, as shown in Fig. 2(a). The ABCD parameters between port 1 and ports 2 and 3 can be expressed as

Fig. 2

(a) Equivalent circuit of proposed divider when port 1 is excited and (b) equivalent circuit of the proposed divider when port 2 is excited.

(2) (A21B21C21D21)=(cos θ1LjZuL·sin θ1Lj sin θ1LZuLcos θ1L)

(3) (A31B31C31D31)=(cos θ2LjZuL·sin θ2Lj sin θ2LZuLcos θ2L)(10j tan θ3LZuL1)

The ABCD parameters of Eqs. (2) and (3) can be converted into the S-parameters of S₂₁ and S₃₁. Using the relation of S₂₁ =k·S₃₁, the following related equations are then obtained.

(4) k2RcTRbT·(RbT+1+k2k2RaT)cos θ1L={RcT+(1+k2)RaT}cos θ2L-RcT sin θ2L tan θ3L

(5) k2RcTRbT·(ZuL2+1+k2k2RaTRbT)sin θ1L={ZuL2+(1+k2)RaTRcT}sin θ2L+(1+k2)RaTRcT cos θ2L tan θ3L

In Fig. 2(a), under the input matching condition (S₁₁ = 0), we have

(6) 1Z2e+1Z3e=1RaT

(7) Z2e=ZuLRbT+jZuL tan θ1LZuL+jRbT tan θ1L

(8) Z3e=ZuLRcT(1-tan θ2L tan θ3L)+jZuL tan θ2LZuL+jRcT(tan θ2L+tan θ3L)

where Z₂_e and Z₃_e are the input impedances of the upper and lower branches, respectively.

Based on the principle of conservation of energy and ideal transmission lines, the real parts of Z₂_e and Z₃_e are expressed as follows:

(9) Re[Z2e]=1+k2k2RaT

(10) Re[Z3e]=(1+k2)RaT

In Fig. 2(b), when port 2 is excited, the networks of Net1 and Net2 are connected in parallel, in which Net1 consists of the isolation resistor R_iso and the transmission line of electrical length θ₃_L; and Net2 consists of a termination resistor R_aT and transmission lines of electrical lengths θ₁_L, θ₂_L. The ABCD parameters of Net1 and Net2 can be expressed as:

(11) (ANet1BNet1CNet1DNet1)=(1Riso01)(cos θ3LjZuL sin θ3Lj sin θ3LZuLcos θ3L)

(12) (ANet2BNet2CNet2DNet2)=(cos θ1LjZuL sin θ1Lj sin θ1LZuLcos θ1L)(101RaT1)(cos θ2LjZuL sin θ2Lj sin θ2LZuLcos θ2L)

The ABCD parameters of Eqs. (11) and (12) are converted into the Y-parameters of Net1 and Net2, respectively, and the admittance parameters of the entire network can be obtained as follows:

(13) (y11_toty12_toty21_toty22_tot)=(y11_Net1y12_Net1y21_Net1y22_Net1)+(y11_Net2y12_Net2y21_Net2y22_Net2)

where

y11_tot=cos θ3LRiso cos θ3L+jZuL sin θ3L+cos θ1L cos θ2L-sin θ1L sin θ2L+jZuLRaTsin θ2L cos θ1L-ZuL2RaTsin θ1L sin θ2L+jZuL(sin θ2L cos θ1L+sin θ1L cos θ2L),
y12_tot=y21_tot=-1Riso cos θ3L+jZuL sin θ3L+-1-ZuL2RaTsin θ1L sin θ2L+jZuL(sinθ2L cos θ1L+sin θ1L cos θ2L),
y22_tot=cos θ3L+jRisoZuLsin θ3LRiso cos θ3L+jZuL sin θ3L+cos θ1L cos θ2L-sin θ1L sin θ2L+jZuLRaTsin θ1L cos θ2L-ZuL2RaTsin θ1L sin θ2L+jZuL(sin θ2L cos θ1L+sin θ1L cos θ2L).

The admittance parameters of Eq. (13) can be converted to the S-parameters of S₂₂, S₃₂, and S₃₃ with terminated impedances of R_bT and R_cT. The S-parameters of the entire network between ports 2 and 3 can be expressed as

(14) S22=-(y11_tot-1RbT)(y22_tot+1RcT)-y12_tot·y21_tot(y11_tot+1RbT)(y22_tot+1RcT)-y12_tot·y21_tot

(15) S32=-21RbT·1RcT·y21_tot(y11_tot+1RbT)(y22_tot+1RcT)-y12_tot·y21_tot

(16) S33=-(y11_tot+1RbT)(y22_tot-1RcT)-y12_tot·y21_tot(y11_tot+1RbT)(y22_tot+1RcT)-y12_tot·y21_tot

Based on Eqs. (4) to (5), (9) to (10), and (14) to (16), the electrical lengths θ₁_L, θ₂_L, θ₃_L, and isolation resistance R_iso that satisfy the power divider characteristic conditions with |S₂₂| < −20 dB, |S₃₃| < −20 dB, and |S₃₂| < −20 dB at center frequency can be obtained by using MATLAB.

III. Simulation and Experimental Results

To validate the proposed power divider, we designed two types of circuits at a center frequency of 2 GHz. One has a power dividing ratio of k² = 2 and port impedances of R_aT = 40 Ω, R_bT = 70 Ω, and R_cT = 60 Ω. The second circuit has a power dividing ratio of k² = 4 and port impedances of R_aT = 50 Ω, R_bT = 70 Ω, and R_cT = 60 Ω. For the first circuit, when the transmission line characteristic impedance of Z_uL = 40 Ω was chosen, we calculated the electrical lengths and isolation resistance using the equations above and after optimization as follows: θ₁_L = 157^o, θ₂_L = 146^o, θ₃_L = 47^o, and R_iso = 12 Ω. For the second circuit, when a transmission line characteristic impedance of Z_uL = 40 Ω was chosen, we calculated the electrical lengths and isolation resistance using the equations above and after optimization as follows: θ₁_L = 153°, θ₂_L = 130°, θ₃_L = 66°, and R_iso = 20 Ω. The Teflon substrate of the proposed power divider had a dielectric constant of 2.5, a thickness of 0.787 mm, and a conductor thickness of 0.035 mm.

The simulation was performed using Microwave Office software with version 13 developed by National Instruments.

Fig. 3(a) and (b) show the photographs of the circuits in which k² = 2 and k² = 4, respectively, where power dividers of various port impedances and uniform transmission lines are implemented. For the measurement, the impedance transformers shown in Fig. 3 were used to match the input and output ports to 50 Ω.

Fig. 3

Photographs of the implemented power divider: (a) k² = 2 and (b) k² = 4.

Fig. 4(a) and (b) show the measured and simulated S-parameters of the circuit with a power dividing ratio of k² = 2 and port impedances of 40, 70, and 60 Ω; the figures show insertion losses of |S₂₁| = 2.0 dB and |S₃₁| = 5.0 dB, an isolation of |S₃₂| > 25 dB, an input return loss of |S₁₁| that is better than −20 dB, and output return losses of |S₂₂|, |S₃₃| that are better than −18 dB at the center frequency of 2 GHz. In addition, Fig. 5(a) and (b) show the measured and simulated S-parameters of the circuit with a power dividing ratio of k² = 4 and port impedances of 50, 70, and 60 Ω; the figures show insertion losses of |S₂₁| = 1.2 dB and |S₃₁| = 6.8 dB, an isolation of |S₃₂| > 25 dB, an input return loss of |S₁₁| that is better than −25 dB, and output return losses of |S₂₂|, |S₃₃| that are better than −25 dB, −13 dB, respectively, at the center frequency of 2 GHz. In Figs. 4 and 5, the |S₃₃| data can be observed with slight frequency deviation, which is caused by the parallel admittance of electrical length θ₃_L. Fig. 6 shows that the phase difference between the output ports of the k² = 2 circuit is +3° at the center frequency of 2 GHz. Table 1 shows a comparison of dividers using the conventional uniform transmission line and the results obtained for the proposed divider. In addition, Table 2 summarizes the experimental results and design parameters of the proposed power divider.

Fig. 4

Measured and simulated S-parameters of the k² = 2 circuit: (a) |S₂₁|, |S₃₁|, |S₃₂| and (b) |S₁₁|, |S₂₂|, |S₃₃|.

Fig. 5

Measured and simulated S-parameters of the k² = 4 circuit: (a) |S₂₁|, |S₃₁|, |S₃₂| and (b) |S₁₁|, |S₂₂|, |S₃₃|.

Fig. 6

Measured and simulated phase difference between the output ports of the k² = 2 circuit.

Table 1

Comparison of the proposed divider with conventional power dividers

Table 2

Summary of experimental results and design parameters of the proposed power divider

IV. Conclusion

This paper presented a modified Wilkinson divider using uniform transmission lines for various terminated impedances and an arbitrary dividing ratio. With this configuration, the desired splitting ratio can be obtained by adjusting only the electrical length of the transmission lines between the ports. Moreover, it has the advantage that the impedance of the ports is set to various terminated impedances, and is connected to a circuit without a matching circuit. The feasibility of the proposed power divider design concept was demonstrated, and the simulated and measured results were confirmed to be in good agreement.

References

1. Wilkinson EJ. An N-way hybrid power divider. IRE Transaction on Microwave Theory and Techniques 8(1):116–118. 1960;

2. Gysel UH. A new N-way power divider/combiner suitable for high-power application. In : Proceedings of IEEE MTT-S International Microwave Symposium. Palo Alto, CA; 1975. p. 116–118.

3. Kim Y, Yoon YC. A modified unequal power divider with a complex isolation component for enhanced isolation. Microwave and Optical Technology Letters 57(2):322–324. 2015;

4. Agrawal AK, Mikucki GF. A printed circuit hybrid ring directional coupler for arbitrary power divisions. IEEE Transactions on Microwave Theory and Techniques 34(12):1401–1407. 1986;

5. Ahn HR, Wolff I, Chang IS. Arbitrary termination impedances, arbitrary power division and small-sized ring hybrids. IEEE Transactions on Microwave Theory and Techniques 44(12):2241–2247. 1997;

6. Ahn HR, Wolff I. Three-port 3-dB power divider terminated by different impedances and its application to MMICs. IEEE Transactions on Microwave Theory and Techniques 47(6):786–794. 1999;

7. Cheng KKM, Li PW. A novel power-divider design with unequal power-dividing ratio and simple layout. IEEE Transactions on Microwave Theory and Techniques 57(6):1589–1594. 2009;

8. Li PW, Cheng KKM. A new unequal power-divider design with enhanced insertion loss flatness. IEEE Microwave and Wireless Components Letters 19(12):786–788. 2009;

9. Haiwei Z, Quan X. A novel Gysel power divider with arbitrary power ratio for high-power application. In : Proceedings of IEEE International Wireless Symposium (IWS). Beijing, China; 2013. p. 1–4.

10. Zhu YZ, Zhang XF, Wu XF, Li C, Fang GY. Novel Wilkinson power divider with uniform impedance line. In : Proceedings of Asia-Pacific Microwave Conference (APMC). Macau, China; 2008. p. 1–4.

11. Horst S, Bairavasubramanian R, Tentzeris MM, Papapolymerou J. Modified Wilkinson power dividers for millimeter-wave integrated circuits. IEEE Transactions on Microwave Theory and Techniques 55(11):2439–2446. 2007;

12. Qi T, He S, Dai Z, Shi W. Novel unequal power divider with 50 Ω characteristic impedance lines. IEEE Microwave and Wireless Components Letters 26(3):180–182. 2016;

13. Lin F, Chu QX, Wong SW. A novel Gysel power divider design with uniform impedance transmission lines for arbitrary power-dividing ratios. Journal of Electromagnetic Waves and Applications 27(2):242–249. 2013;

14. Park MJ, Lee B. Design of ring couplers for arbitrary power division with 50 Ω lines. IEEE Microwave and Wireless Components Letters 21(4):185–187. 2011;

15. Eom DS, Lee HY. A broadband half-mode substrate integrated waveguide quadrature Wilkinson power divider using composite right/left-handed transmission line. Journal of Electromagnetic Engineering and Science 17(1):9–13. 2017;

Biography

Young-Chul Yoon received his B.S., M.S., and Ph.D. in electronics engineering from Sogang University, Seoul, Korea, in 1978, 1982, and 1989, respectively. In 1987, he joined the Department of Electronics Engineering, Catholic Kwandong University, Gangneung, Korea, where he is currently a Professor. His areas of interest are the design of high power amplifiers for the ISM band, and RF and microwave circuit analysis and design.

Young Kim received his B.S., M.S., and Ph.D. in electronics engineering from Sogang University, Seoul, Korea, in 1986, 1988, and 2002, respectively. He developed cellular and PCS linear power amplifiers at Samsung Electronics Co., Ltd. In 2003, he joined the School of Electronics Engineering, Kumoh National Institute of Technology, Gumi, Korea, where he is currently a Professor. His areas of interest are the design of high-power amplifiers and linearization techniques, and RF and microwave circuit analysis and design.

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