Balun Designs for Wireless-Mixers-Amplifiers and Antennas

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    Balun Designs for Wireless

    M ixers, Am plifiers and Antennas

    BalunsJind w ide use in mixer antenna and balanced amplzJier circuits yet their

    design is not widely practiced. The author shows a variety of designs that are simple

    and yield go od first pass results.

    Rick

    Sturdivant

    Hughes Aircraft C ompa ny

    El Segundo California

    aluns find wide use in mixer, antenn a and bal-

    anced am plifierc ircuits. Yet balun design is still

    regarded as if

    t

    were black magic by many

    enginee rs, partly due to the fact that practical design

    information on baluns can be difficult to find. How-

    ever, many good baluns have been dev eloped over the

    years and som c are surprisingly simple to design. In this

    paper we will review somc good balun designs and

    show that good first pass design results can be obtained .

    Balun circ uits find wide application espe cially in new

    wireless applications as they have customarily in

    R F

    and microw ave circuits. They a re used in circuits such

    as mixers, push-pull amplifiers, antennas and other

    applications requiring a conversion between unbal-

    anced transmission line such as coa x, stripline or

    microstrip) and a balanced line such as a two wire

    transmission line of the type used for old television

    antenna leads).

    A

    properly de signed balun is essential for these types

    of circuits. In fact, it is often the perform anc e of the

    balun which predominately determines the perfonn ance

    of the overall circuit.

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    Interestingly, the design of balun s is rarely covered in

    most engineeringcurriculum. Furthermore, the design

    information o n them is scattered throughout a num ber

    of different articles. T he goal of this paper is to save the

    circuit designer time by cataloging a few good balun

    designs.

    str p

    Balun

    Theory

    housing

    dielectric

    supp rt

    ~h~

    purpose of

    a halull

    i s

    to forln good transition

    Figure 2 Shielded parallel plate line is a balanced transmission

    line

    from an unbalanced transmission line into a balanced

    transmission line. Figure illustrates coax, a familiar

    unbalanced line. The current I exists on the center

    conductor, I, is the ground return for

    I

    and Ie is the

    externa l current induced on the outs ide of the shield.

    The shield is considered tied to earth ground at the

    input.

    A shielded parallel plate line, on the other hand , has

    equal potential and 180 degree s of phase difference

    between the current on the two conductors. with no

    curren t on the ground shield. Th is is illustrated in Figure

    2. The currents are I,=-I,, and I, is the ground return.

    I

    exists only w hen the eclual am plitude and op posite phasc

    relationship between

    I

    and I, is not maintained. Ic s thc

    induced external current on ihe outside of the shield.

    To speak of the potential at the balanced end of thc

    circuit referenced to gr o~ lnd s unnecessary, since it is

    the potential between the balanced pair of co~lductors

    which is responsible for the transmission of power along

    them.In fa ct, for the theoretically perfect balu n, an ideal

    current sourc e placed betw een one of the balanced lines

    and ground w ill produce zero current in that line.

    How ever, for many mixe r and amplifier designs it is

    not necessary to have a theoretically perfect balun. That

    is, many circuits do not require the infinite ground

    isolation property of the ideal balun. Rathe r, these

    circuits only require that the voltages on the balanced

    lines are of equal magnitu de and opposite phase , and

    that the impedance to ground may be finite but equal

    for both conductors). Baluns have been developed over

    the years which meet this requirement. These quasi

    baluns are the m ajor focu s of this article.

    Half Wave

    Tran,s.missionLine

    Possibly the simplest balun is show n in Figure 3. The

    phase sh ift of 180 degree s which is required for balun

    operation is achieved by a half wavelength piece of

    transmission line. Impedance tnatchin gcan be achieved

    by properly choosing the impedance of the halfwave

    line. This is an inherently narrow band design . A

    quarter wave transformer can be added at the unbal-

    anced input to improve thepe rfom ~an ce. his circuit is

    designed by modifying the line impedance of the half

    wave and quarter wave line i f used) to achieve the best

    performance.

    unb l nced =--

    e

    end view side view

    Figure

    I

    Coaxial line is an unbalanced transmission line

    Figure

    3

    Simple half wavelength balun

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    N

    Sections

    o Halj

    Wave Lines

    Lumped Element Balun

    By interconnecting anusnber of halfwavelength trans-

    mission lines with quarter wavelength lines (Figure

    41

    wide band baluns are possiblc[l]. The bandwidth can

    be i~lcrcascci y adding more sections. The order,

    n

    o f

    the balun depends upon the nurnber

    of

    halfwavelength

    sections. The half wavelength lines provide the 180

    degrees of phase shift while the quartel- wavelength

    lines give the impedance transformations. This is a

    balun design that is practical in tnicrostrip. Due to its

    planar structure the circuit pattern can beetchedon only

    one side of the substrate.

    balanced

    output

    Figure 4 N section halfwave balun

    An n=2 form of this balun has bccn dcsiglied and

    tested. The cleinent lengths and isnpedances have been

    optimized. The measured performance is shown in

    Figure

    5 .

    Return Loss

    4

    Isotat~on

    lnsertlon

    Loss

    lnse~t lon oss

    Baluns can be do igncd by using lu~np ed lemenh.

    Lumpcd clement baluns are well suited for low frc-

    quency and

    MMIC

    applications[2],[3] for which dis-

    tributed linc lengths would be too bulky. The theory of

    lusnped clesne~lt aluns i5 based upon the familiar rat

    race ring hybrid. The distributecl transini\\ion line4 of

    the rat race ring are replaced by lu~npedelement quiva-

    lent circuits. The quarter wave length lines of the ratrace

    ring are replaced by lumped element lowpa5s f~ lt er

    networks. The three quarter wavelength line is replaced

    by a highpaus filter network. The resultant equivalent

    lumped element circuit is shown in Figure

    6. The

    required design equations arc included.

    where:

    o

    = I/(oC) = 1.4 4 K

    R = Port Impedance

    w = center frequency (rad/sec)

    Figure

    6

    Lumped element balun

    The theoretical pel-forniance of this balun is shown in

    Figure 7. A 50 ohm load was assunled on all ports.

    Therefore,

    C

    0.325pF and

    L

    1.125pF.

    Parallel Plate Balun

    Of all the baluns in use today possibly the most widely

    used is the quarter wave coupled line balun. There are

    many configurations for it. The broadside coupled

    parallel plate balun is very common[4]

    [ 5 ] , [ 6 ] .

    t is

    6

    7 1 Sound in Inany mixel-designs and is shown in Figure 8

    requency

    [GHZJ

    It consists of an input rnicrostrip line which transitions

    into parallel plate line. The parallel plateline is adoublc

    Figure

    5

    Measured performance of n=2 half

    wave

    balun

    sided substrate.

    38

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    Return Loss

    . . . . s x Insert on Loss

    Lsolatlon

    Insert lot Loss

    a magnetic wall 15 placed between the balanced lincs.

    Their neth hod, which

    i

    bawd on the variational tech-

    nique, is 5traight forward and easy to pro gram .

    9 1 2

    1 3

    Frequency

    [GHz]

    Figure 7. Theoretical perform anceofth e lumped element balun.

    Figure

    8.

    Parallel plate balun. Backside contluctor shown as

    dashed lines topside conduc tors as solid lines.

    A taper is usually a dded to the backside g ro ~u id lane

    to aid in the mo dc conversion from microstrip to parallel

    platc. H owev er, relatively

    good

    performance is possible

    without using a taper ifth e eve11mode

    impedance

    is very

    large cornpared to the odd mod e impe danc e. Usually

    soft sub strates a]-euseci for the sup port dielec tric and a re

    usually very thin (5mil typically).

    A s ide view of the balun is shown in F i p r c 9. The

    parallel platc region is actua lly a pair of coupled line s.

    T h c ev e n an d o dd ~ n o d c nalysis; ca n be do ne using th e

    tcchniyue devclopcd by Bhat andK o~1 1[7 ]osthe analy-

    s is o f br oads id e co ~ ~ p l e du sp end ed s ~ ~ b s t r a t etripline

    (BCSS S) . The odd impedance,Zoo. is the charac teristic

    impedance ofon e

    of

    the baliunced conducto rs to groun d

    when shorting plane is placed at the symm etry line

    between the balanced conductors . Thc even mode i n -

    pedance is the character ist ic irnpcd~it lce ne ~z s i ~r edc-

    tween on e of the balanced conductors and ground when

    On e of the benefits of the parallel platc balun is that it

    is possible to ach lev e grouncl isolation at the balanced

    outpu ts. That is the balancccl lincs have the ir potential

    refcrcnccd to each other, with near Lero potential be-

    tween either balanced linc and ground.

    Figure 9. Side view o f the parallel plate balun.

    I lie actual parallel plate im ped anc e(Z op) is twice the

    BCSSS odd mod e impedance. Therefore, the impcd-

    ance u5edfor the design of the b alunis rclatcd totheocid

    node BCSSS impedancc by

    W he reZ op 1s the parallel platc impe dance . In order to

    have a good match at the rnicrostrip inpu t, we must have

    Equation 1 z

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    5 7 8

    9

    10 11

    Frequency

    [GHz]

    Figure

    10

    Frequency response of the parallel plate balun

    A parallel plate balun was used in the design of am ixe r

    realized on 25 mil alumina (er=9.8). Th e performan ce

    is good for a first cut design. The design called for a

    mixer with a bandwidth covering 8-10 GH z with less

    than 9dB conversion loss. The port

    VSWR was less than

    2:

    1

    using the balun configuration shown in Figure with

    no taper to the trace on the back sides of the substrate.

    The conversion loss as

    a

    function of the r.f. frequency is

    shown in Figure I .

    6 5 7 0 7 5 8 0 8 5 9 0 9 5 10 0 10 5 11 0

    R F

    frequency[GHz]

    Figurc

    11

    Conversion loss of the singly balanced mixer

    Microstrip Coupled Line Balun

    Adesign similarto the parallel plate baluncan bem ade

    using coupled microstrip. Thc design procedure uses

    Equations 1-3. This type of balun has performance

    similar to that shown in Figure 10. How ever, the

    condition of Equation 3 can be difficult to satisfy in

    microstrip.

    Using only two coupled lines does not usually give

    enough coup ling to achieve good performan ce, better to

    employ three. A typical layout for this balun is shown

    in Figure 12. T he two lines which couple to the center

    strip are shorted at the unbalanced input and attached

    periodically by jumper wires. This short circuit causes

    the capacitance between these two strips and the ground

    plane to be shorted out. Transform ing a quarter wave

    length to the balanced o utput causes the im pedance to be

    very large (theoretically an open circuit).

    via

    t

    ground

    unbalanced balanced

    via t o

    ground wires

    Figure 12 Microstrip balun using coupled lines where the

    coupled region is a quarter wave length long for the odd m ode

    Marchand Balun

    A wide band balun which has been used for years is the

    Marchand balun[8J. Many exam ples of the Marchand

    balun can be found in the literature [8,9,10]. Figu re 13

    is an exam ple of a coaxial line Marchand balun.

    balanced

    Gutput

    Figure 13 Marchand balun in coax

    Published analyses suggest that bandwidths ap proach-

    ing 50:

    1

    heoretically are possible. The author is aware

    of realizations yielding bandwidths o f

    :

    1. The design is

    amena ble to both coax and microstrip media.

    A

    quasi Marchand balun is shown in Figure 14. This

    is not a true Marchand balun du e to the fact that the even

    mode impedan ce between the coupled lines is defined

    between eac h line and ground. With this embodiment

    there is a finite (even m ode impe dance) between the

    non-groun ded lines and ground. This is an additional

    impedance not represented in Marchand s balun. The

    predicted pe rformance is shown in Figu re

    15

    For Zoo

    35 ohm and Zoe = 250 ohm and 5 0 ohm loads on the

    ports.

    42

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    balanced

    unb l nced

    7 7

    Zoe Zoo Zoe Zoo

    -

    Figure

    14.

    Quasi Marchan d balun u sing coupled lines.

    -- eturn

    LOSS

    -.-- -

    Insertion loss

    4 8

    1

    1 2 4 1 6

    8

    Frequency [GHz ]

    Figure

    15.

    Calculated response of the quasi M archand balun.

    eferences

    [ l ] B M ayer, R Knoechel, Biasable b alanced mixers and frequency

    doublers using a new planar balun, Conference Proceeding: 20th

    European M icrowave Con ference. V2, 1990 , pp. 1027- 1032.

    121 S amue l P a r ~ s ~ ,Monolr th~c,umped e l ement , wg l e vdebnnd

    modulator, 1992 IEk E M TT-S lnterrldl~ondlM l c r o ~ve Sqmpo-

    ~ l u m ~ ges t , p 1047-1050

    [3] S. J Par~sr , 180 dcgrcc lumped elenlent Hy b~ld . 1989 IEEE

    MTT-S Intcmat~ondlMicrownvc Syrnpos~umDrgest, Vol 3. pp.

    1243-1246.

    141

    C. Y. Ho, New analysis tccllniquc builds bcttcr baluns .

    Microwaves and RF, Aug., 1985. pp. 99-102.

    [S]

    B .

    Clinier, Analysis of suspended microstrip taper baluns,

    Proc. IEE. Vol. 135, Pt H. No. 2 April 1988, pp. 65-69 ,

    161 S. Padin, B. Arend. G. Narayanan, A ~ [id cb an dSB mixcr using

    high I'l-ecluency operatio nal amplifiers. Micro wav e Journ al. March

    1992. pp. 131-133.

    [7] B.

    Bhat and S.K. Koul. Unified approach to solve a class of strip

    and microstrip-like transmission lines, IEEE Trans. Microwave

    Thcory Tcch.. vol. MTT-30, pp. 679.686, May 1982.

    181

    N .

    Marchand, Transrnisiion line conversion transformers.

    Electronics, 1944, 17. pp. 142- 145.

    [9] J.W . McLauphlin.

    R.W.

    G r o ~ ,A w~ de-bandb,tlun. IRE

    Trans.. 1958. MTT, pp.

    3

    14-316.

    LIO] K

    Rawer.

    J .J .

    Wolfe. Aprin tedcircuit balun for use with spiral

    antennas, IKE trans., 1950, MTT , pp. 3 19-325.

    Rick Sturdivant l.ec,ei~>ed

    ile

    BA D e-

    Col orr~ioColleg e arrd tlle BS 6E L)e-

    I [

    L011,q HCLIC.IIll 1989. In 1992 he

    1c.s.

    111 1989 Irejo it~eiItk e atkrr Sys retn.~

    G ~ , O L I I I

    t

    H ~ ~ g 1 ~ e . sir-~ .rtf t s u Me~rrl-

    h e ri ft lr e ~ ' t ~ ~ ~ / l t l i c ~ u ~ S t u j j :r-eseirtly lr

    i . \ ra.q~oi~sihlr

    iw

    tha de.\.ig/~f high

    clc~nsit? ~ic.ro+r.u~.c,uc .kugc~sf ir p-

    pIic.crtiot1 to ro ilu t.sy ~rc ~n7 s.VIlilr irt H u g h r ~7r 1zci s hrc~tl.c~.s~~orl.sihle

    for IR &D pr.~jo(. ts 11 rnir~i(ltur-e~ir.(.lll(~tur..~r1i1di~~1eser . srld tlle

    design

    r?f kllC.s

    or EEW otld ?wuTur- sj st en ls . H is ir1rerests tr1.c irl

    mict.o\ta\'epocku,yin,q, nrlcl tkc desig n i~f fi'lter-s,ili.rer.s, ntld circlr la-

    tor.s.

    Rick is a rrlcnlhc/ of T a u Beta P i , aridE t i~ N O ~ NU .

    44

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