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    For internal circulation amongst members only.

    2006, Vol . 1

    Inside this Issue

    Fox Hunt SpecialButterfly Handi-finder

    3 element 2M yagi

    BITX20 SSB XVR

    What is Sporadic E ?

    Published by :

    Calcutta VHF AmateurRadio Society

    PresidentDeepak Mitra VU2DPM

    Vice PresidentJ ayanta R. Mukherjee VU2J M

    SecretaryNikhilesh CH. Sinha, VU2NKI

    TreasurerSurojit Kr. Dey, VU2SKD

    EditorNilanjan Majumdar VU2HFR

    website :www.calcuttahams.com

    Locating Hidden Transmitters - Radio Direction FindingA "fox", which is a low power transmitter set to transmit a tone or ID for a set

    length of time, and then goes silent until its time to transmit again. By using

    various radios and antennae and attenuating systems, the teams start out from a set

    start line to locate the "fox". The first team to locate the "fox" is the winner. (The

    "fox hole", which is the location of the transmitter and the "fox howl", which isthe tone or id transmitted from the transmitter).

    Objective: To develop radio direction finding skills, foster the construction ofradio direction finding tools, and have a good time through competition and social

    interaction. Designed to be a fun event for all.

    General rules: The location, the game frequency and the call frequency should bedetermined before the start of the fox hunt. The fox howl should be copied at the

    starting point by the majority of the hunters present. The fox howl will be at a

    regular interval of every 5 minutes duration, in omni direction for one minute. The

    fox transmitter should maintain constant power throughout the hunt. The antenna

    may not be changed during the course of the hunt. The fox antenna and

    transmitter shall be within 500 feet of access by standard passenger cars in a

    publicly accessible area with no charge for admission. Reasonable care must be

    taken to ensure that hunters can safely get to the hidden fox. The fox may not

    simultaneously transmit another signal to interfere with the fox. The fox must alsomonitor the talk-in (Call) frequency to collect drop outs and announce if he is

    having technical difficulties. A good map of this area should be available among

    the hunters. The hunters can ask the first clue one hour before the end of the

    game, from the game controller who will be available in the call frequency and

    also the second clue 30 minutes before the end of the game. At the end of the fox

    hunt, the game controller will announce the fox hole and the winners. There

    should not be any QSO at the game frequency. The fox hunt may be on vehicle or

    on foot.

    ON THE AIRJournal of the Calcutta VHF Amateur RadioSociety

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    The first and only fox hunt in Calcutta

    was held in 1995 and was organised by

    CVARS. VU2EM won the event using

    this butterfly handi-finder that was built

    by VU2KFR and VU2HFR the Fox

    Brothers who had been the fox during

    the hunt. An article on this handi-finder

    based on the design by Bob Leskovec,

    K8DTS and the article published in the

    May 1993 issue of QST was published

    in the society's journal "On The Air". It is

    high time we had another fox hunt in the

    city to home in our Dfing skills and have

    a field day. In our fox hunt special are

    two articles on the handi-finder and a

    portable plumber's delight 3 element

    VHF yagi which are quite easy to

    construct and give excellentperformance.

    The HANDI-Finder is a hand heldDirection Finder which can be used to

    localize both AM and FM sources using

    only a single connection to the antenna

    input of a VHF-FM receiver tuned to

    the frequency of interest.

    The HANDI-Finder is a good example

    of integrated simplicity, wherein one

    simplification contributes to another.

    First, it uses a single CD4047B CMOS

    IC, which contains both an oscillator

    and a divider flip-flop to automatically

    provide complementary symmetrical

    square wave outputs without special

    adjustments. Only a single resistor and

    capacitor are needed to set the

    frequency. Second, very little current is

    used to bias the switching diodes so the

    total current draw is only 1.7mA at 9V.

    Good service can therefore be provided

    by a common alkaline transistor radio

    battery. Supply voltage for the

    CD4047 can be anywhere from 3-18

    volts. Finally, since all the parts,including the battery are mounted on a

    single circuit board, the board is

    designed to also serve as the mounting

    base for the two open-loop antenna

    elements easily made out of bent wire.

    until later if you really want to!

    HOW IT WORKS: An electronicswitch alternately connects two

    antennas to the coax cable downlead

    going to the antenna input of an FM

    radio receiver tuned to the frequency of

    interest. First one antenna is connected,

    then the other, etc., back and forth with

    equal intervals. This is done at an audio

    rate, well within the audio bandpass of

    the receiver, and usually in the range of

    400 to 1500 Hz. A good frequency is

    1000Hz. Of the two antennas, if one is

    slightly closer to the source, it receives

    the wave front slightly earlier in time

    (phase) than the other. There is a phase

    difference in the signal received by one

    antenna compared to the other. Since

    the receiver is being switched between

    the two antennas, the switching action

    imposes phase modulation on the

    incoming signal. This is detected in the

    FM receiver and is heard at the audio

    output as a tone equal to the switching

    frequency. The amplitude of the audio

    The Butterfly Handi-finder

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    signal corresponds to the deviation,

    which depends on the physical

    separation of the two antenna elements,

    up to wavelength. In other words, if

    the antennas are farther apart the circuit

    will impose a higher percentage of

    modulation or a larger deviation,

    producing a louder tone, but the

    modulating frequency will stay the

    same. If the antenna is rotated so that

    the plane of the two elements isperpendicular or broadside to the

    direction of the signal, both elements

    receive the signal at the same time

    (phase) and there is no longer a

    difference in phase. Hence, the audio

    tone disappears. This is perceived as a

    rather sharp null in the audio as the

    antenna array is rotated into position

    perpendicular to the direction of the

    signal. This type of direction finder has

    the disadvantage that it exhibits 180-

    degree ambiguity. However, it has

    several advantages:

    1) It works on a nulling principle rather

    than a peaking principle. The null is

    sharp and much easier to detect than the

    peak from a directional or beam

    antenna.

    2) When you null the superimposedaudio, you are not nulling the carrier.

    This is unlike a conventional loop

    antenna or cardioid array, which nulls

    out the carrier. The problem with

    carrier-null, is that as you get closer to

    the null, the signal you are trying to hear

    in order to null out, is getting harder to

    hear! Also, when you null the

    superimposed audio, you can still hear

    the audio coming from the source.

    3) Since audio is being nulled, the

    operator does not have to watch a field-

    strength meter. He only needs to listen,

    which is something he can do while

    driving, riding a bike or walking.

    4) Since this method uses phase

    information, it works well with strong

    signals, so no attenuator is required. (By

    comparison, the signal from directionalgain antennas must be progressively

    attenuated to keep the receiver RF

    within the range of the S-meter.)

    The values of C1 and R1 determine the

    switching frequency and hence the

    frequency of the audio tone. The inset

    table shows the values of C1 and R1 to

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    be used for a particular frequency and

    corresponding tone. Very little current

    to bias the switching diodes D1 and D2,

    so the total circuit drain is 1.7 mA at

    9V. No power on LED is used as even

    an LED uses 10 mA or more. The 9-volt

    battery holder is fastened at one end by

    soldering the two brass terminal tabs

    that pass through the board. The switchS1 is a DPDT slide switch (on-off-on).

    Centre is off, up for DFing and down is

    standby mode for straight receiving.

    DONOT TRANSMIT THROUGH THE

    UNIT EVEN ON STANDBY MODE

    AS THIS COULD BLOW THE

    SWITCHING DIODES AND THE

    SWITCHING SYSTEM DOES NOT

    MAINTAIN A 50 OHM IMPEDANCE.

    As the antennas have no path to circuit

    there is no need for using DC blocking

    capacitors. I used two simple copperwire antennas having the appearance of

    butterfly wings soldered directly to the

    board. Take equal lengths of stiff wire

    about 19 inches long and bend each of

    them into a neat U shape. The bottom of

    the U should be 6 inches across. One

    end of the U is soldered to the junction

    of D1 and R4 at one end of the board

    and the other end soldered to the other

    extremity of the board 6 inches from the

    previously soldered end of the U. This

    end of the U is electrically isolated and

    floating and should not be grounded.

    Grounding the other end creates a

    closed loop that results in a carrier null

    in the direction of the signal. Brass or

    brazing rod may be used. It is very

    important that both the loops and the

    associated circuitry should be identical

    and symmetrical and the values of all

    resistances and capacitances on both

    sides should be the same. The active

    element is the vertical portion of the

    loop. The longer the vertical section, the

    more signals it receives and hence better

    carrier strength and better quieting. You

    can experiment with better and highergain antennas such as two identical

    dipoles or yagis connected to both sides

    with equal lengths of coaxial cable.

    The handle should be attached to the

    bottom area of the circuit board ( I had

    used a plastic scale). You can also fix a

    compass on the handle. The unit works

    best when 1/4 wavelength of the

    feedline is kept vertical and parallel to

    the centre of the board. Measure the 1/4

    wavelength feedline from the floating

    antenna terminal. The feedline should

    be taped securely to the handle.

    TRYING IT OUT: It is best to start off

    with a test situation where you knowthe location of the source, and

    experiment with getting a feel for the

    null. The null itself is fairly sharp, but it

    does not always manifest itself as a total

    null in the audio tone. Sometimes, you

    will observe instead, a jump in tone one

    octave up or down. At other times, you

    may hear a buzz or a fast twiddle.

    This is usually due to multipath, so

    moving just a few feet may help clear

    up the null. Calibrate the unit in an open

    field by walking in a circle around a

    central signal source. Never test orcalibrate the unit indoors. Happy DFing

    and Fox Hunting. One last tip:

    DURING A HUNT NEVER TRUST

    WHAT THE OTHER HUNTER SAYS.

    Sense The Right Way To GoWith The HANDI-Finder

    by Joe Moell KOVARRL Technical AdvisorThe following was submitted to theTechnical Correspondence column in

    QST Magazine for October 1993 inresponse to the HANDI-Finderconstruction project in a previousQST issue. The original HANDI-Finder was created by Bob LeskovecK8DTS. The KOV unidirectional

    pattern modification and antennaimprovements described below areapplicable to all of these bow-tie sets.

    Add a Sense Mode

    By adding time delay to the signal from

    one of the two HANDI-Finder antennas,

    the peak/null tone pattern of the unit is

    modified. If you add just the rightamount of delay, the pattern changes

    from bidirectional with nulls

    perpendicular to the antenna plane to

    cardioid (heart-shaped) with a single

    null off one end. This two-pattern

    technique forms the basis of the Handy

    Tracker, a RDF unit that I designed in

    1989. The cardioid pattern concept

    came from an unpublished 1980 project

    by Russ Andrews K6BMG. The Handy

    Tracker sense mode scheme can be

    applied to the K8DTS HANDI-Finder

    with the simple addition of a switch anda length of coaxial cable to provide

    delay. As K8DTS points out, the

    bidirectional HANDI-Finder indication

    is independent of frequency. This is not

    true of the added sense mode. A delay

    line of a given length produces a precise

    cardioid pattern at only one frequency.

    A useful pattern is obtained over a

    frequency range of several per cent,

    however, so one delay line will provide

    ambiguity resolution over one full VHF

    amateur band.

    Modification Details

    The modification adds a DPDT micro-

    mini toggle switch without center-off

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    and a precisely trimmed coax delay line.

    Mount the switch in the etch-free area

    of the circuit board between the two

    antennas.

    On the rear side, cut the traces where C6

    and C7 connect to the antenna terminalsper the drawing. On the Antenna #2

    side, wire the antenna connection

    through the switch per the schematic.

    On the Antenna #1 side, install an

    unshielded wire jumper 1-3/4 inches

    long, to compensate for the added

    switch wiring on the Antenna #2 side.

    This jumper is important, since one inch

    of difference in feed length to one

    antenna will cause 6.5 degrees bearing

    error in the figure-8 bidirectional mode.Cut the delay line according to the

    following formula:l = (11808-df)v/f

    where l = length of coax in inches, v =

    velocity factor of coax as a fraction, f =

    frequency in MHz, and d = spacing

    between the vertical antennas in inches.

    For example, assume we are adding the

    sense mode to a HANDI-Finder with

    "bow tie" open loop antennas for two

    meters. The vertical sections of the two

    loops are 15 inches apart. We are using

    RG-174 coax, which has velocity factor

    of 65.9 per cent. Computed for the

    center of the band (146 MHz), delay

    line length is(11808-(15)(146))(0.659)/146

    = 43.4 inches.

    Coil up the coax and lace it to the board.

    Miniature coax such as RG-174 is best

    for the delay line because it makes a

    compact coil. Whatever coax you use,

    make sure to determine its characteristic

    velocity factor. It is different for foam

    and non-foam type cables.

    Because of environmental multipath and

    stray coupling, a perfect cardioid tone

    pattern may not be achieved. The end

    null may not be complete or there maybe a double null on one end. This

    doesn't matter, because the purpose of

    the sense mode is merely to determine

    which of the two figure-8 nulls to

    follow. There is plenty of peak/null

    amplitude difference for that.

    Getting RDF bearings with the modified

    HANDI-Finder is a simple two-step

    process. In a clear location, with S2 set

    for normal (bidirectional) mode, listen

    for the tone nulls in the receiver to

    obtain a line of bearing as described by

    K8DTS. Next, switch S2 to the cardioidpattern mode and turn the unit 90

    degrees so that one end points along

    your line of bearing. Note the tone level.

    Rotate the unit 180 degrees and note the

    tone level again. It should be distinctly

    different. The lower amplitude tone will

    occur when Antenna #1 is closest to the

    signal source. To help you remember,

    mark the peak/null directions on the

    board.

    Other Observations

    In the K8DTS QST article photo, the

    receiver feedline passes over the open

    end of one antenna loop. This

    unbalances the antenna pair and can

    cause major bearing errors on two

    meters and above. The coax should be

    routed away from the loop.

    The horizontal sections of the bow tie

    antennas severely degrade RDF

    performance. Properly spaced coax-fed

    vertical dipoles are far better for serious

    use with this type of RDF set. Such an

    antenna set is easy to make with

    inexpensive whip antennas and PVC

    plumbing parts.

    The two antennas should be spaced as

    widely as possible for maximum audible

    df tone, but spacing must not exceedone half free-space wavelength at the

    receiving frequency. Approximately 24

    inch spacing is practical for both two

    meters and 125 cm. Coax cables from

    the HANDI-Finder board to each of the

    two vertical dipoles must be exactly

    equal in length.

    Wide antenna spacing gives better

    performance, but it may increase the

    received tone deviation to the point that

    the receiver "squelches out." If this

    occurs, reduce the tone oscillator

    frequency to 400 Hz or lower byincreasing the value of R1 and/or C1.

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    The following design was published in

    the April, 1993 issue of QST. It can also

    be found in the 1996 issue of the ARRL

    Handbook.

    This 3 element yagi is nothing more

    than a half-wave dipole antenna (the

    driven element) mounted between the

    other two elements which are the

    reflector and the director. Typically the

    reflector is 5% longer and the director

    5% shorter than the driven element. By

    spacing elements about 0.15 to 0.25

    wavelengths from each other you end

    up with a beam antenna with about 7dB

    of gain. To figure out the correct length

    of the driven element the following

    simple formula for a half-wave antennaabove 30 MHz is used :

    Length in feet = 475 / Frequency (MHz)

    Construction : 3/4 inch PVCplumber's pipe is recommended for the

    supports. Two 18 inch pieces become

    the boom where the elements are

    installed. A 36 inch piece is used for the

    mast. The boom and mast pieces are

    held together with a PVC T joint. Three

    small holes are drilled in the T as well

    as the boom and mast pieces. The boom

    and mast are inserted into the T androtated until the holes are aligned.

    Screws are used to secure everything in

    place. The antenna is vertically

    polarized which is best for FM work.

    Inexpensive elements can be made from

    steel oxyacetylene welding rods or brass

    rods. The director and reflector

    elements are cut as according to the

    lengths in the diagram. Director and

    reflector holes are drilled in the boom

    around 1/4 or 1/2 inch from each end.

    A straight pencil line should be drawn

    along the boom with an X mark for eachhole to keep the holes aligned at the

    same plane. The hole size chosen should

    provide a snug fit for the rods when

    pushed through. After drilling the

    reflector and director elements are slid

    through the holes and adjusted for equal

    length on each side of the boom. Solder

    or epoxy cement is used to hold them in

    place. To construct the driven element

    the boom is measured and marked at adistance of about 16 inches from the

    reflector. Two holes are drilled 1/8 to

    1/4 inches apart. Two rods each around

    20 inches in length are pushed through

    the holes until 1/4 inch protrudes from

    each side of the boom. THE DRIVEN

    ELEMENT AND MATCHING

    DEVICE HAS JUST BEEN MADE.

    The coaxial cable is soldered directly to

    the protruding stubs. Solder or epoxy is

    used to secure the rods to the boom.

    Electrical tape or a silicon compound is

    used to weather proof the solder joints.It is better to keep a little excess lengths

    for the driven elements. The antenna

    should now be hoisted to an elevation of

    at least 5 feet from the ground and kept

    away from nearby metal objects. With

    the aid of an accurate SWR meter

    placed in the line between the

    transceiver and the antenna the driven

    element lengths should now be trimmed

    equally for the lowest SWR at the

    desired frequency.

    2M 3element yagi designed by Nathan Loucks, WB0CMT

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    BITX20 is a bidirectional SSBtransceiver for the 20m amateur radioband, designed and built by AshharFarhan, 2004. The project details are onhttp://www.phonestack.com/farhan/bitx.html

    You may also join the BITX Yahoogroup at :http://groups.yahoo.com/group/BITX20This group exists for constructors of theBITX project, to discuss all aspects ofthe design and construction includingproblems, components, modificationsand experiences using the rig. TheBITX20 transceiver design has gainedtremendous popularity amongst Indianas well as international Amateur Radiooperators. The circuit boards for thesame are even available with FarCircuits, USA. Joining the yahoo groupgives access to a wealth of informationon the BITX20 including all themodifications made by VU and DX hamsincluding artwork for double sided PCB,overlay and solder mask. This is anexcellent project for both the novice aswell as the experienced avidhomebrewer.

    BITX is an easily assembled transceiver

    for the beginner with very cleanperformance. Using ordinary electronic

    components and improvising where

    specific components like toroids are not

    available, It has a minimum number of

    coils to be wound. All alignment is non-

    critical and easily achieved even

    without sophisticated equipment. The

    entire instructions to assemble the rig

    are given here along with relevant

    theory. The Indian hams have often

    been handicapped by a lack of low cost

    equipment to get them on air. A mono-

    band, bidirectional design usingordinary NPN transistors was developed

    to cater to this demand. The design can

    be adapted to any particular ham band

    by changing the RF section coils and

    capacitors and the VFO frequency.

    BITX evolved over one year from the

    excellent S7C receiver described in the

    new ARRL book Experimental

    Methods in RF Design ( an ARRL

    publication ) into a bi-directional

    transceiver. Several hams across the

    globe contributed to its design. A series

    of emails were exchanged with OM

    Wes Hayward (W7ZOI) during theevolution of this design. His

    contributions have been invaluable. He

    urged me to strive for higher

    performance from the simple design.

    The resultant rig has sensitive receiver

    capable of strong signal handling, a

    stable and clean transmitter capable of

    enough power to make contacts across

    the World. All the parts used in BITX

    are ordinary electronic spares

    components. Instead of expensive and

    hard-to-get toroids, we have used

    ordinary tap washers. Broad-bandtransformers have used TV balun cores.

    The entire transceiver can be assembled

    in India for less than Rs.300. I have

    designed a single side PCB with large

    tracks that can be easily etched at home

    or by any PCB shop. Modificationsand improved compact PCB artwork,component placement guide andoverlays are available at the BITX20

    yahoo group. You may join thisgroup at :http://groups.yahoo.com/group/BITX20for a wealth of information.

    For those who don't readlong articles ...

    There are a couple of things you should

    know before you start assembling the

    circuit:

    The same amplifier block isused throughout. But the

    emitter resistors vary in some

    of the places. Double check the

    values. If you swap values, the

    circuit wont stop working. It

    will work terribly. That might

    be a little difficult to diagnosein the end. Check the emitter

    values and the resistors that go

    between the base and collector.

    The receiving IF amplifierbetween the filter and theproduct detector is coupledto the product detectorusing a 100pf (not 0.1uf).

    BITX20An easy to build 6 watt 20M Bi-directional SSB Transceiver

    by Ashhar Farhan

    http://www.phonestack.com/farhan/bitx.htmlhttp://www.phonestack.com/farhan/bitx.html
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    The crystal filter worked forme, I used crystals from the

    local market marked as KDS.

    These are the cheapest and

    they work with the capacitor

    values given in the filter. Your

    crystals might require a

    different set of capacitors. Try

    the values given here, if youfind the bandwidth too narrow,

    decrease the capacitances, if

    you find it too open then

    increase the capacitances.

    The microphone is directlycoupled to the amplifier as my

    headset microphone needs 5V

    bias. If your microphone works

    without bias, then insert a 1uf

    in series with the microphone.

    The pictures show myprototype on two boards. Dont

    do that, split up the VFO into aseparate box.

    The pre-driver is built onto themain board. The driver and the

    PA are on a separate board.

    Keep the same layout to keep

    the PA stable.

    There is a 50uf on the powerline soldered near the BFO,

    don't forget it. It cleans up the

    audio noise which would

    otherwise get into the receiver.

    On the PCB, there are jumpers

    between T lines and R linesacross the ladder filter. There

    is a jumper from the BFO

    supply to the VFO supply.

    Development Notes

    Bi-directional SSB transceivers have

    been quite common in amateur

    literature. A transceiver was described

    in the ARRL SSB Handbook using

    bipolar transistors. W7UDMs design of

    bidirectional amplifier (as the basis of

    bidirectional transceiver) is referred to

    by Hayward and DeMaw in their bookSolid State Design. The bidirectional

    circuitry is often complex and not

    approachable by the experimenter with

    modest capability (like me).

    The broad band bi-directionalamplifierMy current interest in bidirectional

    transceivers arose after looking at an

    RC coupled bidirectional amplifier in

    the book Experimental Methods in RF

    Design (p. 6.61). An easily analyzed

    circuit that was simple and robust was

    required. It began its life as an ordinary

    broad-band amplifier:

    In any bipolar transistor, the current

    flowing from the collector to emitter is a

    multiple of the current flowing from the

    base to the emitter. Thus, if there is a

    small change in the current flowing into

    the base, there is a bigger change in the

    current flowing into the collector. What

    follows is a highly simplified

    explanation of working of the above

    amplifier.

    In the above circuit, imagine that a

    small RF signal is applied through Rin to

    the base of Q1. Also imagine that the Rfvoltage is swinging up. The transistor

    will accordingly amplify and increase

    collector current causing more current

    to flow through the Rl (220 ohms)

    collector load. This will in turn drop thevoltage at the collector. The drop in

    voltage across the collector will also

    result in a drop at the base (base voltage

    is a fraction of the collector voltage due

    to the way the base is biased). This

    circuit will finally find balance when

    the increase in base current flowing

    from Rin is balanced by the decrease in

    base current due to the voltage drop

    across Rl. In effect the RF current

    entering from Rin flows out through the

    feedback resistance (Rf). The impedance

    seen at the base is effectively very lowand the signal source will see an

    approximate input impedance of Rin.

    Thus, Vin/Rin = Vout/Rf(Eq.1)

    Another factor to consider is that that

    emitter is not at ground. At radio

    frequencies, it looks like there is a 10

    ohms resistor between the emitter and

    the ground. Thus, when the base voltage

    swings, the emitter will follow it. The

    AC voltage variations across the Re (10

    ohms) will be more or less the same as

    that across the base. The current flowing

    into the emitter will mostly consist of

    collector current (and very little base

    current). Thus, if the emitter current

    almost equals collector current,

    Ie = Vin / Re = Vout / Rl (Eq. 2)We can combine these two equations to

    arrive at:

    Vout / Vin = Rf / Rin = Rl / Re. (Eq. 3)

    This is an important equation. It means

    several things. Especially if you just

    consider this part:

    Rf/ Rin = Rl / Re. (Eq 4)

    Lets look at some interesting things:

    1. The voltage gain, and the input and

    output impedances are all related to

    resistor values and do not depend upon

    individual transistor characteristics. We

    only assume that the transistor gain issufficiently high throughout the

    frequencies of our interest. The precise

    value of the transistor characteristics

    will only limit the upper frequency of

    usable bandwidth of such an amplifier.

    This is a useful property and it means

    that we can substitute one transistor for

    another.

    2. The power gain is not a function of a

    particular transistor type. We use much

    lower gain than possible if the transistor

    was running flat out. But the gain is

    controlled at all frequencies for this

    amplifier. This means that this amplifier

    will be unconditionally stable (it wont

    exhibit unusual gain at difference

    frequencies).

    3. You can restate the eq 3 as Rf * Re =

    Rl * Rin . That would mean that for a

    given fixed value of Rf and Re, the

    output impedance and input impedances

    are interdependent. Increasing one

    decreases the other and vice versa! For

    instance, in figure 1, Rf = 1000, Re = 10,

    if we have Rin of 50 ohms, the output

    impedance will be (1000 * 10)/50 = 200

    ohms. Conversely, if we have an Rin of200 ohms, the output impedance will be

    50 ohms!

    In order to make bidirectional

    amplifiers, we strap two such amplifiers

    together, back to back. By applying

    power to either of amplifiers, we can

    control the direction of amplification.

    This is the topology used in the signal

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    chain of this transceiver. The diodes in

    the collectors prevent the switched-off

    transistors collector resistor (220 ohms)

    from loading the input of the other

    transistor. A close look will reveal that

    the AC feedback resistance consists of

    two 2.2K resistors in parallel, bringing

    the effective feedback resistance to1.1K. Thus, the above analysis holds

    true for all the three stages of

    bidirectional amplification.

    Diode mixersThe diode mixers are inherently

    broadband and bidirectional in nature.

    This is good and bad. It is good because

    the design is non-critical and putting 8

    turns or 20 turns on the mixer

    transformer will not make much of a

    difference to the performance except at

    the edges of the entire spectrum of

    operation.The badness is a little tougher to

    explain. Imagine that the output of a

    hypothetical mixer is being fed to the

    next stage that is not properly tuned to

    the output frequency. In such a case, the

    output of the mixer cannot be

    transferred to the next stage and it

    remains in the mixer. Ordinarily, if the

    mixer was a FET or a bipolar device, it

    usually just heats up the output coils. In

    case of diode ring mixers, you should

    remember that these devices are capable

    of taking input and outputs from any

    port (and these inputs and outputs can

    be from a large piece of HF spectrum),

    hence the mixer output at non-IF

    frequencies stays back in the mixer and

    mixes up once more creating a terrible

    mess in terms of generating whistles,

    weird signals and distorting the original

    signal by stamping all over it.

    A simple LC band pass filter that

    immediately follows the diode ring

    mixer will do a good job only at the

    frequencies it is tuned to. At other

    frequencies, it will offer reactive

    impedance that can cause the abovementioned problems. It is requirement

    that the diode mixers inputs and

    outputs see the required 50 ohms

    termination at all the frequencies. In

    other words, they require proper

    broadband termination. Using broad-

    band amplifiers is a good and modest

    way of ensuring that. A diplexer and a

    hybrid coupling network is a better way,

    but it would be too complex for this

    design.

    Circuit Description

    Although simple, every effort was made

    to coax as much performance as was

    possible given the limitations of keepingthe circuit simple and affordable.

    The ReceiverThe RF front-end uses a triple band-

    pass filter for strong image and IF

    rejection. The three poles of filtering are

    quite adequate and the out-of-band

    response of the receiver is only limited

    by external shielding and stray pickups.

    An RF amplifier follows the RF band

    pass filter (Q1) biased for modest

    current. More current would have

    required a costlier transistor. There is

    8mAs through the RF amplifier and thepost-mix amplifiers to keep the signal

    handling capacity of the circuit above

    average. The Post-mix amplifier (Q2)

    does the job of keeping the crystal filter

    as well as the diode mixer properly

    terminated. The crispness of the

    receiver is more due to this stage than

    anything else. An improper post-mix

    amplifier easily degrades the crystal

    filters shape and introduces spurious

    signals and whistles from the diode

    mixer. Note that the mixer is singly

    balanced to null out the VFOcomponent and not the RF port and in

    the absence of proper pre-selection,

    10MHz signals can easily break into the

    IF strip.

    The VFO is fed via a broad-band

    amplifier into the singly balanced

    mixer. We used the simplest VFO

    possible with a two-knob tuning

    mechanism. It works really well and for

    those (like me) used to quick tuning, it

    offers best of both worlds, slow tuning

    through the varactor and fast tuning

    through the capacitor without any slow

    motion drive. Getting a slow motion

    drive is an increasingly difficult

    problem and this is an electrical

    substitute for slow motion drives.

    A word about the VFO: depending upon

    component availability, skills and

    preferences, everybody has a favourite

    VFO circuit. Feel free to use what you

    have. Just keep the output of the

    collector of Q7 to less than 1.5 volts (it

    will appear clipped on the oscilloscope

    trace, that is okay). For 20 Meters

    operation, you will need a VFO that

    covers 4 to 4.4MHz. The given VFO

    has low noise though it does drift a

    little, but I have had no problems with

    ordinary QSOs. After 10 minutes ofwarm up, the drift is not noticeable,

    even on PSK31 QSOs.

    A Hartley oscillator using a FET like

    BFW10 or U310 would work much

    better. You can substitute this VFO with

    any other design that you might want to

    use. If you are using the PCB layout,

    then skip the VFO on board if you want

    to use a different VFO and build it

    externally in a separate box.

    The simple IF amplifier has a fixed

    gain. Earlier it was noted that IF amp

    was contributing noise at audiofrequencies. It was later traced to noise

    from the power supply and placing a

    50uf on the transceiver power line has

    cured it. The IF amplifier has a 100pf

    output coupling to provide roll-off at

    audio frequencies.

    The BFO is a plain RC coupled crystal

    oscillator with an emitter follower. The

    emitter follower has been biased to 6V

    to prevent limiting.

    The detector also doubles up as the

    modulator during transmit mode; hence

    it is properly terminated with an

    attenuator pad. It has no impact on the

    overall noise figure as there is enough

    gain before the detector. The audio pre-

    amplifier is a single stage audio

    amplifier. The 220pf capacitor across

    the base and collector provides for low

    frequency response.

    The receiver does not have an AGC.

    This is not a major short-coming.

    Manual gain control allows you to

    control the noise floor of the receiver

    and I personally find it very useful when

    searching for weak signals or turning it

    down to enjoy the local ragchew.TransmitterThe microphone amplifier is DC

    coupled to the microphone. This was

    done to steal some DC bias that is

    required when using a Personal

    Computer type of headset. If your

    microphone does not require any bias,

    then insert a 1uF in series with the

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    microphone. The microphone amplifier

    is a simple single stage audio amplifier.It does not have any band pass shaping

    components as the SSB filter ahead will

    take care of it all. One 0.001uf at the

    microphone input and another at the

    modulator output provide bypass for

    any stray RF pickup.

    The two diode balanced modulator uses

    resistive as well as reactive balancing. A

    fixed 10pf on one side of the modulator

    is balanced precisely by a variable 22pf

    on the other side. A 100 ohms mini

    preset allows for resistive carrier

    balance. The attenuator pad at the

    output was found necessary to properly

    terminate the diode modulator and keep

    the carrier leakage around the IF

    amplifier to a minimum. While this may

    seem excessive, it produces a clean

    DSB with carrier nearly 50db down

    with careful adjustments on the

    oscilloscope.

    Rest of the transmission circuitry is

    exactly the same as the receiver. Thereis an extra stage of amplification (Q14)

    to boost the very low level 14MHz SSB

    signal from output of the microphone

    tip to driver input level.

    The output amplifier boosts the SSB

    signal to 300mV level, enough to

    directly drive a driver stage.

    The Power ChainA simple power chain consisting of a

    low-cost medium power NPN transistor

    (2N2218) driving an IRF510 for 6 watts

    of power at 14MHz. The output of

    IRF510 uses a tap washer as an output

    transformer. The output transformer has

    40 turns of bifilar winding; these can

    lead to enough stray capacitance to

    affect proper performance as a

    transformer. The half-wave filter that

    follows the transformer absorbs these

    capacitances as a part of the matching

    network.

    I used this power chain because it works

    for me and delivers 6 watts on 14MHz. Idont use more power because I neither

    require more nor do I have a power

    supply that can source more. If you

    need more power, there are a number of

    things that you can do, you can simply

    increase the supply voltage on the

    IRF510 up to 30 volts and extract nearly

    15 watts of power from the same

    configuration. At 30 volts, the drain

    output will be at 30 ohms impedance

    and the pi-network will have to be

    designed to directly match the drain to a

    50 ohms antenna load. Alternatively,

    you could try two IRF510s in push-pull.

    These are variations that you can play

    with. A word of warning though, The

    RF energy at these levels can give you a

    serious RF burn. RF burns can be more

    painful than fire or steam burns. QRP is

    not only fun, it is also safe.

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    ConstructionI would highly recommend that you

    construct it over a plain copper clad

    board by soldering the grounded end of

    the components to the copper and the

    other ends of components to each other.

    Look at the pictures to see how it has

    been done. If you dont know about this

    method of assembling RF circuitry, then

    you should read about it, there are quite

    a few write ups on the Internet about

    this method of RF experimentation. It

    does not require any PCB, it is quite

    robust and very stable.

    Assembling the PCBFor those who feel intimidated by this

    ugly method, I have designed a PCB.

    The PCB layout (component side) is

    provided with this article. It is a single

    sided PCB with wide tracks that can be

    easily made in the home lab. I am

    making a run of these PCBs but

    shipping them abroad (outside India)maybe a problem. Drop a mail to me if

    you are planning to make some PCBs, I

    can put your contact information on the

    website. There are no copyrights over

    either the PCB, the circuit or even this

    article, feel free to copy and distribute.

    The PCB is laid out in a long line.It is 8-

    1/2 inch long and 2-1/2 inch wide. The

    circuit board is big for the circuit that

    goes onto it. This was done so that the

    board is non-critical and it works well.

    All the bidirectional amplifiers are

    similarly laid out.When you get your PCBs, inspect them

    thoroughly, preferable in the Sun.

    Check for small cracks in the tracks.

    Check for tracks that might be touching

    each other or touching the ground plane.

    The PCB layout was done to minimize

    this, but check it anyway. Especially

    check for the tracks that run diagonally

    to the base of each transistor in the

    bidirectional circuitry. These are laid

    out very closely and they are candidatesfor shorting.

    Almost all assembly instructions ask

    you to solder the transistors in the end. I

    would highly recommend that you

    solder the transistors and the diodes

    first. You are most alert when you start

    a project and if you place the transistors

    correctly, the rest of the circuit can be

    soldered around it. Be very careful

    about the orientation of each transistor.

    The microphone amplifier transistor

    (Q10) faces in a direction opposite to

    the rest of the transistors and thetransistor pairs in bidirectional

    amplifiers face each other. The diodes

    have a ring to indicate which way their

    arrow is pointing.

    After the transistors are soldered, finish

    the BFO. If you are assembling this for

    14MHz and above, the BFO will need a

    coil in series with the crystal (USB

    mode), if you are need LSB operation,

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    you will need a trimmer instead (see the

    schematic). Apply power to the BFO

    and you should be able to hear it on

    your Short wave broadcast radio around

    31 meter band. It will sound like a silent

    radio station. It should be quite strong.

    Switching the BFO power supply onand off will help you identify your BFO

    signal on the radio. If you have an RF

    probe, or an oscilloscope, you should be

    able to see the oscillations. Expect RF

    of 2 volts or more.

    Next, assemble the VFO. Winding 150

    turns of the VFO coil is one of the most

    tedious jobs while assembling this rig. It

    has to be done, so just dig in and do it.

    You dont have to attach the 365 pf

    tuning capacitor yet. Check the

    oscillations on a receiver or a frequency

    counter. You may have to decrease thenumber of turns. Without the 365 pf, the

    22pf trimmer should be able to set the

    VFO to 4.3MHz or so. If the VFO is

    oscillating at a lower frequency, then

    remove some turns from the coil. If the

    VFO is at a higher frequency, add 22pf

    in across the 22pf trimmer (if you are

    using the PCB, solder in from the foil

    side). You will require a wire jumper to

    carry power supply between the VFO

    and the BFO. They are the only stages

    that remain switched on during both

    transmit and receive.

    Assemble the audio pre-amplifier and

    the audio power amplifier and attach the

    volume control. When power is applied

    to the audio stages, touching a finger to

    the base of Q4 should produce static in

    the speaker to move even the most die-

    hard trash metal rockers. Next, assemble

    all the three bi-directional stages! This

    involves lot of soldering. But all the six

    stages are exactly the same. Finish one

    stage at a time. The capacitors are

    symmetrically laid out and all of them

    are 0.1uF with one exception (100pf at

    the output of Q3). Remember that the

    emitter bias resistors are 100 ohms, 220

    ohms or 470 ohms. If you mix up thevalues, the rig will still work but it will

    under perform in the presence of strong

    signals and the transmission will be

    splattered. There are jumpers for T and

    R line across the crystal filter. Solder

    them up and power on the R line and

    then the T line alternatively. The

    emitters of bidirectional stages should

    show 2 volts approximately and the

    collectors should show around 8 volts

    and the switched-off transistor should

    show zero voltage on all the three leads.

    For the moment of truth, solder thethree coils, trimmers and capacitors of

    the RF filter, attach an antenna and

    switch it on! Check that the stages are

    working starting from audio end. If you

    touch the volume controls control pin,

    you should hear AC hum and static. If

    you touch the base of Q4, there should

    be a pretty loud static. Take a lead from

    your VOM and touch Q3, you should

    get very loud static, probably mixed

    with local AM broadcast. Touch the

    base of Q2 with the test lead and you

    should get lesser static as the filter

    allows only 3 KHz of 10MHz through.

    Finally, connect the antenna properly at

    the input of the RF band-pass filter and

    peak up the three trimmers for

    maximum atmospheric noise. Attach the

    365 pf and start tuning around the band,

    peak the RF front-end on a strong signal

    and then tune in a weaker signal and

    peak for maximum clarity (not

    maximum sound).

    An important note: Be sure that youhave connected a proper 50 ohms

    antenna load. The RF filter performs

    correctly only at 50 ohms. If you use a

    long wire to do the initial testing, youwill have to touch up the trimmers again

    for the proper antenna.

    Take a break, spend the evening

    listening to your new homebrew. If the

    CW signals tune to dead beat and rise

    on the other side again, your BFO has to

    move its frequency. For USB, add more

    turns to the coil to the BFO coil, for

    LSB, tweak the trimmer. You should

    have a perfect single signal reception. If

    you tune past the dead-beat of a CW

    signal, the signal should drop out

    completely.Assembling the microphone amplifier

    (Q10) and the output amplifier (Q14)

    will complete the exciter portion of the

    transceiver. To put the transceiver in

    transmit mode, ground the R line and

    apply 12V on the T line. Attach the

    output of Q14 to an oscilloscope but

    dont attach the microphone yet. Null

    the carrier with the 100 ohms preset and

    the 22pf trimmer. Each affects the other

    so you might have to go back and forth

    between the two controls.

    Now plug-in the microphone and speak

    into it. You should be able to see clean

    SSB of between 200 and 300 mV on the

    scope at the output of Q14. Instead of

    the oscilloscope you can use another

    14MHz receiver to test your

    transmission quality. Switch off the

    AGC of the other receiver while setting

    the carrier null. A soft whistle (if you

    can manage) into the microphone is

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    should result in a full carrier at the

    output.

    Next, assemble the power chain. At this

    point, you will need a suitable chassis to

    house your project. Any metal box will

    do. If you dont have any, you can

    solder pieces of copper clad together

    (like I did) and make a U shapedchassis. Keeping the VFO in open air

    makes it drift a bit. A closed box is

    really very useful.

    A big cookie (or chocolate) box of tin is

    really ideal. With a hand drill, you can

    easily make holes to fit the two PCBs

    inside it. Tin is easily soldered on. Use

    the biggest knob you can find for the

    main tuning. The plastic broadcast

    capacitors usually have a very short stub

    that cannot take a big knob. It takes on a

    small plastic drum that is held onto the

    capacitor spindle with a retaining screw.Clip on the drum onto the tuning

    capacitor, tighten the retaining screw

    well and with epoxy glue, stick a big

    knob over the drum. This will make

    your main tuning mechanism.

    I use a simple double pole triple throw

    switch for Transmit/Receive switch-

    over. If you prefer PTT operation, you

    can easily substitute the switch for a

    relay. Be sure to solder a reverse biased

    diode across the relay coil to prevent

    reverse voltage from entering into the

    transceiver power line.

    Use shielded cable for all the

    connections between the power

    amplifier and the main board.

    Tune-up and Operation

    Set the VFO to correctly cover 4.0 to

    4.4MHz. If you can, take your rig over

    to a ham friends shack, you can

    monitor your VFO on his rig at the edge

    of 80 meters band at 4.0MHz. Set the

    trimmer so that you can hear the VFO

    when the friends receiver is tuned to

    4.0MHz and your tuning capacitor is

    fully closed (as much as it will go anti-

    clockwise). After this, connect the

    antenna and peak the RF coils for

    maximum noise in the speaker. If you

    can tune it to a weak signal, then peak

    the RF coils for best reception.

    You might find that although you are

    able to tune in CW stations, you are

    unable to hear the SSB stations

    properly. This indicates that your BFO

    is not properly set. We will take that up

    next.

    On amateur bands above 10MHz, SSB

    is transmitted on upper sideband and on

    bands below 10 MHz, it is transmitted

    on lower sideband. To tune a upper

    side-band signal, your BFO has to be atthe lower edge of the crystal pass-band.

    You will require either the inductor (for

    USB) or the capacitor (for LSB) in

    series with the BFO crystal. If your

    BFO is set to proper frequency then the

    signals will tune in and as you continue

    tuning across the signal, they will drop

    in pitch and disappear. If the signals

    appear muffled, then the BFO is set in

    the crystal filters center, add more turns

    to the coil (USB), or tweak the trimmer

    (LSB). If the signals appear shrill and

    you are unable to zero-beat them, thenthe BFO is too far away from the filters

    frequency - Decrease the coils turns

    (for USB) or tweak the trimmer (LSB).

    The transmitter tune-up essentially

    involves setting the carrier null. It is

    best to tune up the transmitter on a

    dummy load. I use 8 220 ohms, 2 watts

    resistors in parallel as my dummy load.

    It is worth the few bucks to have a

    proper dummy load. Attach the dummy

    load on the transmitter, and attach an

    RF probe to the dummy load (or an

    oscilloscope). As you speak, you should

    get 20 volts or more peak voltage on the

    dummy load when you whistle or just

    go haaaaallow. On another receiver in

    the same room, connect a short piece of

    wire as an antenna and monitor your

    own signal. You will probably be able

    to hear your own carrier as well. Null it

    by tweaking the 100 ohms preset and

    the 22pf balance trimmer. They both

    interact, so you might have to go back

    and forth between the two controls.

    A word of caution, the diode mixers are

    prone to generating odd harmonics. The

    third harmonic of 4 MHz is at 12MHz.So, if you simply peak the coils for

    maximum output on transmit, you might

    wrongly peak the RF front-end to 12

    MHz (I did that). The RF band-pass

    filter is best tuned in receive mode over

    a weak signal at 14.150MHz or so and

    left at that.

    Conclusion

    There might be a kit (components and

    the PCB in a bag) soon. I personally

    dont have the time to put kits together.

    If somebody is interested in doing so,

    just go ahead and do it. The design is

    free, you dont need to ask my oranybody elses permission. The purpose

    is to address the need among Indian

    hams in particular for an SSB rig that is

    easily and cheaply built. My original

    aim was to keep the price under Rs.

    1000. The current design brings the cost

    to well under Rs.300.

    6 Watt Linear PA PCB artwork.

    Modifications / improved compactPCB artwork, component placementguide and overlays are available atthe BITX20 yahoo group. You may

    join this group at :http://groups.yahoo.com/group/BITX20

    for a wealth of information.

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    BITX PCB Artwork andcomponent layout

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    This article has been prompted by the

    DX we often encounter on the VHF

    bands for an understanding of how

    and why the S21 stations come

    blasting on our beloved 2M band. The

    article is based on the information

    available at

    http://www.g4xgt.co.uk/what-is-

    sporadic-e.htm

    What is sporadic E ?Irregular scattered patches of relatively

    dense ionization that develop seasonally

    within the E region and that reflect and

    scatter radio frequencies up to 150

    MHz. Sporadic E is a regular daytime

    occurrence over the equatorial regions

    and is common in the temperate

    latitudes in late spring ,early summerand, to a lesser degree, in early winter.

    At high, i.e., polar, latitudes, Sporadic E

    can accompany Auroras and associated

    disturbed magnetic conditions. It can

    sometimes support reflections for

    distances up to 2,400 km. Sporadic E is

    a form of propagation that can arise

    with little warning, and enable radio

    frequencies of 150 MHz and more to

    travel over distances of a thousand

    kilometres and more. Many people

    experienced it in the days of the old

    VHF television transmissions. Whensporadic E propagation arose, it would

    result in severe interference to the

    signals. Even now VHF FM broadcasts

    in the 88 - 108 MHz band can be

    affected. In many instances the arrival

    of Sporadic E can cause unwanted

    interference as signals that are normally

    too distant to be heard appear. However

    for radio amateurs it offers the chance to

    make contacts over much greater

    distances than are normally possible.

    Sporadic E arises when clouds ofintense ionisation form in the region of

    the E layer. These clouds can have very

    high levels of ionisation, allowing

    frequencies up to about 150 MHz to be

    reflected on some occasions. The clouds

    are usually comparatively small,

    measuring only about 50 to 150

    kilometres in diameter. Their shape is

    irregular. Sometimes they may be

    almost circular, whereas others may be

    long and thin. They are also surprisingly

    thin, often only measuring a few

    hundred metres in depth.

    These clouds appear almost at random,

    although there are times when they aremore likely to occur. They form in the

    day, and dissipate within a few hours.

    They are also far more common in

    summer, peaking approximately in mid

    summer. As they form the level of

    ionisation gradually builds up, affecting

    first the lower frequencies, and later

    higher frequencies as the level of

    ionisation increases.

    Propagation via sporadic E occurs in the

    same way as normal ionospheric

    propagation. Signals from thetransmitter leave the earth as a sky-

    wave, travelling towards the ionosphere.

    Here they are reflected (or more

    correctly refracted) back to earth where

    they are heard at a considerable distance

    from the transmitter. Like normal

    ionospheric propagation it is the free

    electrons that affect the signals, causing

    them to bend back towards the earth. In

    view of the fact that the sporadic E

    clouds occur at around the same height

    as the E layer, similar distances are

    achieved. Typically the maximum

    distances are about 2000 km.

    It is found that the sporadic E ionisation

    clouds move. Being in the upper

    atmosphere they are blown by the winds

    in these areas and can drift at speeds of

    up to 300 kilometres per hour. This

    means that when sporadic E is being

    experienced, the area from which

    stations are heard will change over the

    life of the cloud.

    Theories

    There are many theories about sporadicE and how it occurs. Some believe that

    it may be related to thunderstorms,

    others think it results from the winds in

    the upper atmosphere. None of these

    theories have been established, leaving

    the reasons behind sporadic E a

    mystery, and predictions of when it will

    occur have to be left to statistics.

    However even though the mechanism

    behind the formation of sporadic E is

    not fully known it is still possible for

    radio amateurs to utilise them to enable

    them to make contacts over long

    distances

    What is Sporadic E ?

    Wouldn't it be lovely to haveanother Fox Hunt in the city.The last and only one that wehave had so far was held wayback in 1995. Time foranother one !! This edition of"On The Air" carries simpleDF gear designs that anyonecan brew. The society has

    received permission to changeits registered name from"Calcutta VHF AmateurRadio Society" to "BengalAmateur Radio Society." Ifthe resolution for the same ispassed at the EGM on 5thMarch, 2006 the society'sname will be changedpermanently. There are plansto have an annual event in the

    form of a Fox Hunt this year.So gear yourselves and letshave a gala time at the 2006Fox Hunt.

    "On The Air" published by :Calcutta VHF Amateur RadioSociety9, Mandeville Gardens

    Apt - 5FKolkata - 700 019www.calcuttahams.comEmail : [email protected]

    Editor: Nilanjan MajumdarVU2HFR