A Wideband, Varactor-tuned Microstrip VCO

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    A Wideband, Varactor-tuned Microstrip VCO

    The design of a varactor-tuned VCO covering an octave frequency range up to 4 GHz and more

    By Matjaz Vidmar

    June 01, 1999

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    ICUWB 2012 (September 17, 2012 - September 20, 2012)

    A Wideband, Varactor-tuned Microstrip VCO

    Matjaz Vidmar

    University of Ljubljana

    Slovenia

    When electrical tuning of an oscillator is required over a wide microwavefrequency range, yttrium iron garnet (YIG)-tuned oscillators usually provide the

    widest frequency coverage as well as relatively low phase noise. While YIG-

    tuned oscillators generally provide a tuning range of more than one octave, the

    tuning range of varactor-tuned VCOs is much more restricted. Furthermore, all

    available varactors are rather lossy capacitors with low Q values at frequencies

    above 1 GHz, degrading the phase noise of the oscillator.

    Wideband, varactor-tuned microwave VCOs are usually built as hybridmicrocircuits to reduce device parasitics. Expensive GaAs varactor chips are

    used to simultaneously increase the frequency coverage and reduce the phase

    noise due to the better Q of GaAs varactors when compared to their silicon

    counterparts. Although varactor-tuned VCOs cannot compete with YIG VCOs

    directly, significant improvements can be made with a better varactor-tuned VCO

    circuit design.

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    This article presents the design of a varactor-tuned VCO covering an octave

    frequency range up to 4 GHz and more. The VCO design uses standard surface-

    mount device (SMD) components, including inexpensive silicon varactors.

    Furthermore, the VCO is built using conventional microstrip technology on

    inexpensive FR-4 circuit-board laminate. Finally, the phase noise of the described

    VCO is reasonably low (approximately 20 dB worse than a free-running YIG

    oscillator).

    Wideband VCO Design

    Wideband VCO design with negative-resistance active devices

    is difficult due to circuit parasitics. Two-port amplifier devices

    offer the designer more freedom. A basic microstrip oscillator

    design with a two-port amplifying device is shown in Figure 1.

    Any oscillator design requires an amplifier and a frequency-selective feedback

    network. Besides the desired frequency response, the feedback network should

    also provide the correct phase shift so that the total phase shift in the feedback

    loop equals an integer multiple of 360. Of course, this total phase shift also

    includes the phase shift inside the active device, which is usually much larger

    than 180 due to device and package parasitics at microwave frequencies.

    In the case of a microstrip oscillator, the feedback network may include aninterdigital bandpass filter to determine the oscillator frequency. Additional

    phasing microstrip lines are required to bring the total phase shift to an integer

    multiple of 360 at the desired operating frequency. In addition, the feedback

    network should be designed so that oscillation is only possible at the fundamental

    mode of the interdigital bandpass filter, while oscillations at higher order

    resonance are suppressed.

    A fixed-frequency oscillator can be modified into a VCO by inserting one ormore varactors into the circuit. If a single varactor is inserted in series with the

    central finger of the interdigital bandpass, frequency coverage of approximately

    10 percent around a central frequency of 2 GHz can be obtained. Although a

    single varactor may tune the interdigital bandpass over a wider frequency band,

    the desired phase shift cannot be maintained over the wider range to keep the

    oscillator running.

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    A wideband microstrip VCO can be built only if the phase velocities of all

    microstrip lines are controlled. The phase velocity of a microstrip line can be

    controlled using several series or parallel variable reactances distributed along

    the microstrip line. A series connection is usually used at microwave frequencies

    due to the relatively high capacitance of available varactors.

    A tunable microstrip oscillator design is shown in Figure 2.The phase velocity of the microstrip lines is controlled by

    several variable capacitors connected in series in the

    transmission lines. The capacitors adjust both the center

    frequency of the microstrip bandpass filter and the overall

    phase shift of the feedback network. If the spacing between

    adjacent variable reactances is kept sufficiently small (less than one-quarter

    wavelength at the maximum operating frequency), very wide tuning ranges are

    possible.

    A Practical S-band VCO

    The circuit diagram of a practical wideband, varactor-tuned microstrip VCO

    operating in the S-band (2 to 4 GHz) is shown in Figure 3. The

    feedback network includes an interdigital bandpass filter tuned

    with six type BB833 silicon, hyperabrupt varactors (0.75 pF

    minimum capacitance, 1.8 W series resistance, SOD-323 SMDpackage). Several 22 kW resistors are used as resonance-free

    RF chokes to apply the same tuning voltage to all six varactors.

    Due to the low Q of the varactors used, the insertion loss of the feedback network

    is rather high. Therefore, a type BFP420 high ft silicon bipolar transistor (ft = 25

    GHz, SOT-343 SMD package) is required as the active device. The DC bias is

    provided by a simple resistor network. In order to isolate the oscillator, only a

    very small fraction of the RF signal is taken through a resistive divider from thecollector to the output.

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    Some components are required only to simplify the printed-

    circuit-board layout (for example, the series connection of two

    4.7 kW resistors for the base bias). Other components are

    required to suppress unwanted resonances, such as the two 100

    W resistors in the varactor bias circuit. Finally, the VCO is

    followed by two buffer stages to further isolate the output, as

    shown in Figure 4.

    The microstrip circuit was etched on 0.8-mm-thick, double-sided FR-4 glass

    fiber-epoxy laminate. Two different layouts were tested, both

    with dimensions of 20 mm x 80 mm, as shown in Figure 5. The

    narrowband version uses higher impedance microstrip lines in

    the feedback network, resulting in stronger coupling and lower

    insertion loss. The wideband version uses wider microstrip

    lines, resulting in weaker coupling and higher insertion loss, butwith wider frequency coverage using the same varactors. All passive SMD

    components (resistors and capacitors) are standard size 0805 parts.

    If the described VCO is to be redesigned for different frequencies and/or different

    varactors, the circuit size first should be scaled. Second, the center finger of the

    microstrip bandpass should be tuned to obtain the correct phase shift in the

    feedback loop. If tuning of the center finger shifts the operating frequency range

    too much, the entire circuit must be scaled again. Next, tracking of the amplitude

    and phase response should be checked while adjusting the varactor tuning

    voltage. Finally, the amplitude response should be checked both at the desired

    frequency and at the undesired higher order resonances of the microstrip feedback

    network. This design procedure applies equally to computer simulation and

    practical circuit tests.

    The VCO's Measured Performance

    Three versions of the described VCO were built. The first version was built on

    the narrowband PCB 1 with BB833 varactors. The second version was built on

    the wideband PCB 2 (also with BB833 varactors). The third version was built on

    PCB 1 with better BB857 silicon hyperabrupt varactors (very small SCD-80

    SMD package, 0.55 pF minimum capacitance and 1.5 W series resistance).

    Several samples of all three versions were built and tested.

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    The typical tuning curves of all three VCO versions are plotted

    in Figure 6. The first version covers 2 to 3.85 GHz, depending

    on the tolerances of the varactors used. The tuning range of the

    second version is approximately 150 MHz wider, covering 2.05

    to 4.05 GHz with the same varactors. The tuning range of the

    third version extends from 2.4 to 4.6 GHz thanks to the

    improved BB857 varactors.

    The tuning range of all three versions can be extended by approximately 50 MHz

    on the lower end by allowing the tuning voltage to turn negative to -0.7 V. The

    tuning curves are quite nonlinear. The tuning slope exceeds 100 MHz/V at tuning

    voltages of approximately 7 V and falls below 10 MHz/V at tuning voltages of

    approximately 30 V. Since the VCOs were designed for the widest frequency

    coverage, no attempt was made to linearize the frequency/voltage response in the

    RF circuit.

    Since specialized phase noise test equipment was not available, the phase noise

    of the available model HP8593EM spectrum analyzer was first roughly estimated

    The phase noise of the analyzer was determined to be sufficiently low to

    accurately measure the phase noise of the described VCOs. Two samples of the

    first and second versions (with BB833 varactors) were packaged in shielded

    cases and connected to well-filtered supply and tuning voltage sources.

    The single-sideband (SSB) phase plots, shown in Figure 7, demonstrate that the

    described VCOs are roughly 20 dB worse than the YIG

    oscillator inside the spectrum analyzer. Interestingly, the phase

    noise is approximately 5 dB stronger at the band center than at

    the band edges, suggesting that at least part of the phase noise is

    caused by thermal noise voltage generated in the 22 kW

    resistors that is modulating the VCO frequency at the point

    where the tuning slope is the steepest.

    Possible VCO Improvements

    Although the frequency coverage of the described VCO exceeds the advertised

    performance of commercially available hybrid VCOs, many improvements to the

    described circuit are still possible. In particular, the phase noise performance

    probably could be improved. Last, but not least, the described VCO design can

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    be readily adapted to other two-port active devices, such as GaAs FETs, high

    electron mobility transistors, heterojunction bipolar transistors or MMIC

    amplifiers.

    Part of the phase noise is caused by the 22 kW resistors used as resonance-free

    chokes to bring the tuning voltage to the varactors. Lower resistor values cannot

    be used since the RF circuit losses increase. True RF chokes (inductors) shouldbe selected carefully to avoid parasitic resonances in the frequency range of

    interest.

    The phase noise performance could also be improved by replacing the simple

    resistor bias network of the BFP420 transistor. Since the S parameters of bipolar

    transistors depend mainly on the DC bias currents through the transistor, the

    transistor's operating point should be accurately stabilized to further improve the

    phase noise performance.

    Both the phase noise and long-term (thermal) stability of the VCO could be

    improved by using a better microstrip material than the suggested FR-4 glass

    fiber-epoxy laminate. This material has a high temperature coefficient, shifting the

    VCO frequency downwards by a few megahertz for each degree of temperature

    increase. Besides lower temperature coefficients, suitable microwave substrates

    should also provide lower losses and higher Qs for the microstrip resonators.

    The nonlinear frequency/voltage response of the described

    VCO design may require a linearizer. A simple tuning slope

    linearizer circuit is shown in Figure 8. The gain of the two

    operational amplifiers is set to the lowest value around the

    reference voltage of +7 V DC (where the VCO tuning slope is

    the steepest). At lower and higher tuning voltages, some

    positive feedback is switched in so that the overall gain increases to compensate

    for the decay that occurs in the tuning sensitivity.

    The requirements for the linearizer response could also be estimated form the

    varactor diode capacitance (CT = f(VR)) curves shown in Figure 9. Curves for

    the BB833 and BB857 varactors clearly show that the maximum relative

    capacitance change occurs between 5 and 10 V. Above 15 V, the capacitance

    curves become flat, resulting in a decrease in the VCO's tuning slope.

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    The presettable potentiometers P1 to P8 permit the switching points to be set.

    Since the upper part of the tuning curve is much more nonlinear

    than the lower part, six switching points are used in the upper

    part (resistors R+) and only two switching points are used in the

    lower part (resistors R-). Besides using low noise operational

    amplifiers, the resistor values should be selected carefully to

    avoid excessive noise generation in the linearizer circuit (resistor values too high)or excessive power dissipation (resistor values too low).

    Conclusion

    A varactor-tuned VCO has been designed that uses standard SMD components

    and inexpensive silicon varactors. The VCO's frequency tuning range is over one

    octave and extends above 4 GHz. The VCO is built using low cost FR-4 PCB

    material and achieves good SSB phase noise performance.

    Acknowledgment

    The author wishes to thank Knut Brenndoerfer of Siemens Semiconductors,

    Munich, Germany, for supplying the many different varactors and other SMD

    semiconductor samples without which the described VCO could not have been

    developed.

    Matjaz Vidmar received his BSEE and MSEE from the University of Ljubljana,

    Slovenia in 1980 and 1983, respectively. He received his PhD in 1992, also

    from the University of Ljubljana, for developing a single-frequency GPS

    ionospheric correction receiver. Vidmar is currently teaching undergraduate

    and postgraduate courses in electrical engineering at the University of

    Ljubljana. His current research includes high speed electronics for optical fiber

    communications. Vidmar is also taking part in amateur satellite projects. He

    developed very high efficiency VHF and UHF transmitters that weresuccessfully flown in space on the Microsat mission in 1990.

    Recent Articles by Matjaz Vidmar

    Microstrip Resonant Phase Shifters

    A Microwave Analog Frequency Divider

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