A Reduced-size Power Divider Using the Coupled Line Equivalent to a Lumped Inductor
A new method of reducing the size of a power divider using quarter-wave length transmission lines is proposed. The method utilizes a combination of shorted coupled lines instead of lumped inductors and capacitors. The new hybrid is simply fabricated wi...
In many applications, such as balanced power amplifiers, mixers and antenna systems, power dividers/combiners are required. Power dividers using quarter-wave lines become prohibitively large at the lower frequencies and result in MMIC chips of larger size and higher cost. The lumped-element approach, which uses lumped inductors and capacitors, is one of the solutions to this problem. Inductors for microwave circuits can be realized with air-wound coils; however, such coils must be space-wound with gaps between turns resulting in wide variations in their inductance value.^{1} Spiral inductors represent another possible compromise, although their quality factor (Q) is often sacrificed to obtain adequate inductance. Equivalent lumped-element models for spiral inductors have been obtained from two-port S-parameter measurements. These models do not lend themselves readily to design applications because their elements are difficult to evaluate in advance.^{2,3,4} Gupta and Getsinger^{5} presented a quasi-lumped-element branch-line coupler, which uses lumped capacitors and short-circuited transmission lines as inductors, but the resulting design is inconvenient to fabricate.
In this article, a new miniaturized transmission line technique, using a shorted parallel-coupled pair instead of a microwave inductor, is introduced. It enables the lumped inductor of the power divider to be transformed into a short distributed transmission line. This technique provides flexibility in size.
The Short Coupled Line Equivalent to a Lumped Inductor
The quarter-wavelength transmission line shown in Figure 1 is a key element in power combiners. It can be equated to a combination of a lumped inductor and lumped capacitors. The aim of this study is to obtain a smaller distributed circuit that is equivalent to the lumped inductor in the quarter-wavelength transmission line. With an artificial resonance inserted, the equivalent circuit becomes the one shown in Figure 2 . Figure 3 shows a shorted parallel-coupled line and its equivalent P network, except for a 180° phase difference.^{6,7} The dotted box in the equivalent circuit of a /4 transmission line can be made equal to the shorted parallel-coupled line if the following equations are satisfied:
X_{0} = Z_{oe} tan (1)
X_{L} = {(2Z_{oe}Z_{oo})/(Z_{oe}-Z_{oo})}tan (2)
where
X_{0} = shunt impedance in the network
X_{L} = series impedance in the network
Z_{oe}, Z_{oo} = even and odd impedances of the shorted parallel-coupled line
= electrical length of the shorted parallel-coupled line
= angular frequency
The resultant quarter-wave transmission line is shown in Figure 4 . The capacitor is expressed as
C = {(Y_{0} cot )/ } + {1/( Z_{oe} tan )} (3)
where cot is inserted for X_{L} to be equal to the impedance of C_{1} in the equivalent circuit of a /4 transmission line. For example, in the design of a power divider, the characteristic impedance of the /4 transmission line is X_{L} = 70 and from Equation 2, the following relation is obtained:
Z_{0} = (2Z_{oe}Z_{oo})/(Z_{oe}-Z_{oo}) = X_{L} cot (4)
where
Z_{0} = characteristic impedance for the shorted parallel-coupled line
As the electrical length becomes shorter, the characteristic impedance becomes larger. This trend is similar to the lumped distributed /4 transmission line in which the characteristic impedance of the shorter transmission line proposed by Hirota tends to be high.^{8} In this case, the higher impedance is limited to approximately 100 because the width of the high impedance line becomes too narrow to fabricate and its losses increase. Thus, the transmission line in power dividers could not be shorter than /8. Fortunately, the very high characteristic impedance Z_{0} is easily obtained in a coupled line.^{9} At this point, it becomes necessary to examine the phase variation of a /4 transmission line with frequency, compared to the shorted parallel-coupled line because the artificial resonance gives rise to a narrower band. In the equivalent circuit of a /4 transmission line composed of a shorted coupled line and capacitors, the S_{21} parameter of the /4 line is given by
S_{21} = (-y_{21}Y_{0}/D_{y}) (-1) (5)
where
y = (y_{11} + Y_{0})(y_{22} + Y_{0}) - y_{12}y_{21}
y_{11} = y_{22} = -j Y_{oe} cot -j {(Y_{oo} - Y_{oe})/2} cot + jB
y_{21} = y_{12} = -j {(Y_{oo} - Y_{oe})/2} cot
B = Y_{oe} cot + Y_{0} cot (6)
In Equation 5, the minus value in parentheses shows that there is a 180° phase difference between the network and the shorted coupled section. y_{11}, y_{12}, y_{21} and y_{22} are the y-parameters of the shorted coupled line with the capacitor C in the equivalent /4 transmission line circuit. At the resonance frequency, Equation 6 is satisfied when the characteristic admittance Y_{oe} of the shorted transmission line is equal to the shunt capacitance. With a straightforward analytical manipulation, the equation for the phase of S_{21} can be derived as
Phase of S_{21} = 3 /2 + tan^{-1}x_{1} + tan^{-1}x_{2} (7)
where
x_{1} = B/Y_{0} -2cot - Y_{oe}cot /Y_{0} (8)
x_{2} = (B - Y_{oe} cot )/Y_{0} (9)
Y_{0} = (Y_{oo} - Y_{oe})/2
Near the center frequency, x_{1} and x^{2} are expressed by -cot and cot , respectively, using Equation 6. The phase of S_{21} is -90° at the resonance frequency. If the frequency deviates from the center frequency, the relation C_{0} = Y_{oe} cot cannot be satisfied and the phase of S_{21} starts to deviate from -90°. At this point, the most important item is to decrease the frequency sensitivity of the equivalent /4 transmission line. If Y_{oe} is small, the frequency sensitivity decreases because of the very small shunt value of C_{0} in the artificial resonance circuit. The coupling coefficient K is
K = (Y_{oo} - Y_{oe})/(Y_{oo} + Y_{oe}) (10)
From Equation 10, the following relation is obtained:
Y_{oe} = {(1-K)/(1+K)} Y_{oo} (11)
From Equation 11, when the coupling coefficient is nearly unity, Y_{oe} is very small. The 90° phase shift near the center frequency is independent of the coupling coefficient K. As a result, the larger coupling coefficient K causes the /4 transmission line with a shorted coupled line to be broadened as a function of frequency. Figure 5 shows the final reduced size power divider with shifted coupled line instead of a lumped inductor and lumped capacitor. It is very compact and simple to fabricate.
Table 1 | |||||||
Z _{o} = 250 | = 15.79° | ||||||
K(dB) | -1 | -3 | -5 | -10 | -15 | -20 | -25 |
Zoe ( ) | 2048.75 | 606 | 321.25 | 111 | 53.75 | 27.5 | 14.875 |
Zoo ( ) | 117.812 | 103.625 | 89.986 | 58.792 | 37.587 | 22.541 | 13.293 |
BW (%) | 129.9 | 110.5 | 76.7 | 40.4 | 23 | 12.9 | 7.4 |
Z _{o} = 400 | = 10.024° | ||||||
K(dB) | -1 | -3 | -5 | -10 | -15 | -20 | -25 |
Z_{oe} ( ) | 3278 | 968 | 514 | 183.8 | 86 | 44 | 23.8 |
Z_{oo} ( ) | 188.499 | 165.753 | 143.978 | 95.779 | 60.14 | 36.066 | 21.269 |
BW (%) | 131.3 | 112.5 | 77.7 | 41.6 | 23.4 | 13.1 | 74 |
Z _{o} = 500 | = 8.048° | ||||||
K(dB) | -1 | -3 | -5 | -10 | -15 | -20 | -25 |
Z_{oe} ( ) | 4097.5 | 1212 | 642.5 | 222 | 107.5 | 55 | 29.75 |
Z_{oo} ( ) | 235.624 | 207.25 | 179.922 | 117.585 | 75.175 | 45.082 | 26.586 |
BW (%) | 131.7 | 113.2 | 78 | 41.2 | 23.5 | 13.1 | 7.4 |
Z _{o} = 700 | = 5.767° | ||||||
K(dB) | -1 | -3 | -5 | -10 | -15 | -20 | -25 |
Z_{oe} ( ) | 5736.5 | 1694 | 899.5 | 321.65 | 150.5 | 77 | 41.65 |
Z_{oo} ( ) | 329.873 | 290.086 | 251.961 | 167.613 | 105.245 | 63.115 | 37.221 |
BW (%) | 132 | 113.4 | 78.2 | 41.9 | 23.6 | 13.2 | 7.5 |
Z _{o} = 1000 | = 4.044° | ||||||
K(dB) | -1 | -3 | -5 | -10 | -15 | -20 | -25 |
Z_{oe} ( ) | 8195 | 2424 | 1285 | 444 | 215 | 110 | 59.5 |
Z_{oo} ( ) | 471.248 | 414.501 | 359.944 | 235.169 | 150.35 | 90.164 | 53.172 |
BW (%) | 132.1 | 113.7 | 78.3 | 41.7 | 23.6 | 13.2 | 7.5 |
Z _{o} = 2000 | = 2.025° | ||||||
K(dB) | -1 | -3 | -5 | -10 | -15 | -20 | -25 |
Z_{oe} ( ) | 16390 | 4848 | 2570 | 888 | 430 | 220 | 119 |
Z_{oo} ( ) | 942.496 | 829 | 719.888 | 470.339 | 300.699 | 180.328 | 106.345 |
BW (%) | 132.2 | 113.7 | 78.4 | 41.4 | 23.6 | 13.2 | 7.4 |
Simulation and Experimental Results
Figure 6 shows the bandwidth of the power divider as a function of the shorted transmission line length for various values of K. These simulated results were obtained using the Agilent ADS program. The bandwidth increases as the coupling coefficient K of the shorted coupled line is increased. A peculiar feature is that the bandwidth increases slightly as the electrical length decreases. This is contrary to the results shown by Hirota^{8}, where the bandwidth of the reduced size of the /4 transmission line decreases with its size. The coupling coefficient K has a significant effect on the bandwidth of the power divider. Because of the effect of the coupling coefficient K, the bandwidth of the miniaturized is a strong function of how a tight coupling coefficient can be realized during fabrication. A broadside coupled stripline or a Lange coupler can be used for this application.
Table 1 shows Z_{oe}, Z_{oo} and bandwidth as a function of the coupling coefficient K and characteristic impedance Z_{0}. Since only miniaturized transmission lines are of interest, the table considers only electrical length shorter than 15°. The results show that both Z_{oe} and Z_{oo} are larger as the electrical length decreases for constant coupling coefficients K.
As K increases, Z_{oe} increases abruptly while Z_{oo} increases slowly. Since a large coupling coefficient means a wider bandwidth, it is difficult to fabricate a power divider with smaller and wider bandwidth simultaneously.
An experimental, 1 GHz reduced-size power divider was fabricated with microstrip lines on a Teflon substrate with a permittivity _{r} = 3.5 and a thickness of 0.5 mm. The length of the /4 transmission line with a characteristic impedance of 70 is transformed into a /24 coupled line length with a characteristic impedance of 273 and two capacitors of 7.3 pF. It should be pointed out that, to realize the tight coupling necessary, parallel suspended coupled striplines or a Lange coupler are the best option. However, suspended striplines with broadside coupling are very hard to fabricate because of the connection of the lines and capacitors to ground. The Lange coupler needs RFIC technology to realize the tight coupling. Both approaches lead to higher costs. Since narrow band couplers are also in demand in modern communication systems, a lower coupling coefficient can be used. Therefore, K was chosen to be -10 dB using microstrip lines.
Table 2 | |
Z_{oe} ( ) | 117.233 |
Z_{oo} ( ) | 62.067 |
C (pF) | 7.3 |
L (mm) | 8.09 |
W (mm) | 0.3 |
S (mm) | 0.244 |
The coupled microstrip characteristics used for this case are shown in Table 2 . Figure 7 shows the layout and a photograph of the fabricated power divider. The equivalent inductance of the via-holes in the circuit was difficult to calculate and can explain the difference between simulated and experimental results.10 In order to minimize the via-hole inductance, a 0.5 mm thick microstrip substrate is used. The effect of the via-hole grounding on frequency shift was also taken into account for determining the line lengths. Commercial chip capacitors were used, although it was difficult to obtain the exact values necessitated from the simulation. Some small errors can be caused by these variations in capacitor values. The measured performance of the power divider is shown in Figure 8 .
The measured insertion and return losses are in relatively good agreement with the simulated ones. The slight frequency shift in the return and isolation losses is caused by the inaccuracy of the commercial capacitor and via-hole model. The insertion loss of -3.6 dB is due to conductor loss and the capacitor and via-hole accuracies.
Conclusion
A new method of reducing the size of a power divider, using a shorted coupled line pair instead of a lumped inductor, has been proposed and confirmed through experiments using microstrip lines at 1 GHz. The size of the quarter-wavelength transmission line has been reduced to l/24. The proposed method has the advantage of excellent design accuracy. The length of the transmission line could be reduced further, but the bandwidth becomes too narrow. To design a broad bandwidth requires a very tight coupling and is difficult to realize.
Acknowledgment
This work was supported by grant number R01-2001-00298 from the Korea Science and Engineering Foundation.
References
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In-Ho Kang received his PhD degree from Sogang University, Seoul, South Korea, in 1995. He is now an associate professor in the division of radio and information communication engineering at Korea Maritime University, Pusan, South Korea. His research interests include microwave active devices, particularly PA design and reduced-size passive circuits. He can be reached via e-mail at ihkang@hanara.kmaritime.ac.kr.
Jin-San Park received his BSEE from Korea Maritime University, Pusan, South Korea, and is currently working toward his master's degree. His research includes reduced-size passive circuits. He can be reached via e-mail at wavenice@hanmail.net.