Multiband HF antenna design tool

Linked Dipole Calculator & Antenna Designer

Calculate section lengths for a multiband linked dipole, standard dipole, or inverted-V antenna by frequency.

Enter the HF bands or exact operating frequencies you want to use. The calculator returns the starting cut length for each dipole leg, individual linked sections, link positions, and the complete active antenna length for every band.

Linked dipole geometry

Linked Dipole Calculator

Select an amateur band or enter an exact operating frequency in MHz. Calculated dimensions are practical starting cut lengths for final adjustment after installation.

Antenna type
Bands / frequencies
Select an amateur band or enter an exact frequency in MHz.
MHz
MHz
MHz
Default correction factor for insulated wire: 0.95.
Units
Advanced settings
Wire diameter is recorded as a construction parameter; the calculation uses the selected correction factor.
m
Results

Linked Dipole Section Lengths

Use the calculated dimensions as starting cut lengths. Build both antenna legs symmetrically and leave a small amount of extra wire where practical so the antenna can be trimmed during final tuning.

Section Length Table

Band Frequency Section per leg Cumulative leg length Full active dipole Resonant frequency

Antenna Diagram

For a linked dipole, the inner section is active on the highest-frequency band. Closing the next pair of links connects more wire, increasing electrical length and moving resonance to a lower frequency.

40 meter reference

How Long Is a 40 Meter Dipole?

The required length of a 40 meter dipole depends on the exact operating frequency and the correction factor used for the wire. A dipole cut for the lower end of the 40 m band will be longer than one designed for a higher frequency.

Using a half-wave calculation with a 0.95 correction factor gives the following starting dimensions:

Frequency Total dipole length Each leg
7.000 MHz 20.34 m / 66.74 ft 10.17 m / 33.37 ft
7.100 MHz 20.06 m / 65.80 ft 10.03 m / 32.90 ft
7.200 MHz 19.78 m / 64.89 ft 9.89 m / 32.44 ft

These are starting cut lengths rather than guaranteed final dimensions. Insulation, conductor diameter, installation height, inverted-V geometry, nearby objects, and the local environment can shift the actual resonant frequency.

Calculate another 40 m frequency
Installation geometry

Inverted V Antenna Calculator

An inverted-V uses the same basic half-wave dipole principle, but the feedpoint is supported at the apex while both legs slope downward toward their end supports.

Select Inverted V in the calculator to determine the wire length and installation geometry for a chosen frequency.

Inputs
  • Frequency
  • Wire correction factor
  • Apex angle
  • Center or apex height
  • End height
  • Units
Outputs
  • Total wire length
  • Length of each leg
  • Horizontal span
  • Vertical drop
  • Estimated end height
  • Apex angle

If the entered apex angle and support heights describe incompatible geometry, the calculator flags the conflict instead of presenting misleading dimensions.

Inverted V Length

Changing a horizontal dipole into an inverted-V does not mean simply choosing an arbitrary shorter wire length. Start with the calculated resonant length and allow for practical tuning after the antenna is installed in its intended position.

Lowering the ends changes the antenna environment, feedpoint impedance, radiation pattern, and resonant behavior. This is why final adjustment should be carried out with the antenna at approximately the same mast height and angle that will be used on the air.

Apex Angle and Horizontal Span

For a symmetrical inverted-V with an included apex angle of θ and a leg length of L, the installation geometry can be estimated as:

Horizontal half-span = L × sin(θ / 2)
Vertical drop = L × cos(θ / 2)
Full horizontal span = 2 × horizontal half-span

The end height is then approximately:

End height = apex height − vertical drop

These dimensions help determine whether the antenna will fit between available supports before wire is cut and the mast is erected.

Fundamentals

What Is a Linked Dipole Antenna?

A linked dipole is a multiband resonant HF antenna made from a dipole conductor divided into several sections. Small electrical links or jumpers connect or isolate those sections, allowing the operator to change the active wire length for different amateur bands.

With the outer sections disconnected, only the shortest inner dipole is active. This configuration is used for the highest selected frequency. Closing a pair of links adds the next conductor sections to both legs, creating a longer resonant dipole for a lower-frequency band.

The result is one physical antenna that can provide several full-size dipole configurations without requiring multiple separate antennas.

Linked dipoles are particularly useful for portable amateur radio because they combine several HF bands in a simple wire antenna. Once properly tuned, band changes are made by opening or closing links rather than adjusting a tuner every time the operating frequency changes.

Operating principle

How Does a Linked Dipole Work?

A resonant half-wave dipole becomes longer as frequency decreases. A linked dipole takes advantage of this relationship by placing the shortest resonant section closest to the feedpoint and adding extension sections toward the ends.

Example:

END — 40 m — LINK — 20 m — LINK — 10 m — FEEDPOINT — 10 m — LINK — 20 m — LINK — 40 m — END

For operation on 10 m, the first links are open and only the inner section conducts.

For 20 m, the first pair of links is closed, connecting the next sections.

For 40 m, both link pairs are closed, so the entire conductor becomes active.

The antenna remains mechanically continuous through its insulators and support system even when an electrical link is open. The connector should carry current when closed, but the mechanical tension should be handled by the wire, insulator, cord, or other structural components rather than by a small electrical contact alone.

Construction

How to Build a Linked Dipole

Start by choosing the bands and operating frequencies. A linked dipole designed for specific frequencies is more useful than one based only on nominal band names, especially when most operation will take place in a particular CW, digital, or SSB portion of a band.

Calculate every cumulative dipole length first. The difference between two adjacent cumulative leg lengths becomes the physical extension section between the corresponding links.

Cut both antenna legs as mirror images. Keep the left and right sections equal and provide a practical trimming allowance before final tuning.

Wire and Insulators

A lightweight stranded insulated conductor is convenient for a portable antenna, while other conductor types may be suitable for permanent installations. The important point is to use the same wire assumptions during calculation and construction.

Insulated and bare conductors can resonate at different physical lengths. Wire diameter and insulation can also affect the final result, so the calculator should be treated as the start of the tuning process rather than a substitute for measurement.

Place an insulator at every section break. It must maintain mechanical continuity when the electrical link is open.

How to Make the Links

A link needs to provide a reliable electrical connection while remaining quick to operate in the field.

Possible constructions include:

  • short wire jumpers;
  • banana-style connectors;
  • small removable clips;
  • compact plug-and-socket connectors;
  • other low-resistance connections suitable for the expected RF power and environment.

Arrange the link so that unplugging it does not release the antenna mechanically. Strain should remain on the conductor support and insulator rather than on the electrical connector.

Clearly marking each link can make band changes faster, particularly on a multiband portable antenna.

Feedpoint and Coax

A center-fed dipole is a balanced antenna, while standard coaxial cable is an unbalanced feedline. The feedpoint should provide solid connections to both dipole legs and mechanical strain relief for the coax.

Route the coax away from the feedpoint as cleanly as practical rather than running it directly alongside one antenna leg for a significant distance.

A resonant linked dipole is commonly intended to present an impedance that can be used with a typical amateur transceiver and 50-ohm coaxial feed system, but the actual feedpoint impedance depends on installation geometry and surroundings.

1:1 Current Balun

A 1:1 current balun or effective common-mode choke can help reduce unwanted RF current on the outside of the coax shield.

Without adequate symmetrization, the feedline can become part of the radiating system. This may alter the measured impedance and radiation pattern, contribute to RF in the station, and make tuning change when the coax is moved.

A ferrite-based current choke at or near the feedpoint is one practical way to provide this common-mode suppression.

Portable Installation

A linked dipole can be supported horizontally or as an inverted-V from a portable mast. An inverted-V often reduces the number of high supports required because the feedpoint can be raised on one mast while the ends slope down to separate anchor points.

For field use:

  • label each link;
  • keep both antenna legs symmetrical;
  • prevent connectors from carrying mechanical strain;
  • avoid placing wire ends where people can walk into them;
  • maintain practical clearance from the ground and surrounding objects;
  • tune the antenna using a setup similar to the intended operating configuration.

If links cannot be comfortably reached from the ground, plan a way to lower the antenna for band changes rather than pulling directly on the coax or radiator.

Adjustment

How to Tune a Linked Dipole

Calculated dimensions are starting values. Final resonance should be checked after the antenna is assembled and installed.

The most reliable approach is to tune the shortest, highest-frequency section first and then work outward toward the lower-frequency bands.

Tune the Inner Section First

Open all link pairs so only the shortest inner dipole is electrically active.

Install the antenna at its normal height and, if applicable, its normal inverted-V angle. Measure the resonant frequency with an antenna analyzer.

If resonance is lower than the desired frequency, the active section is electrically too long and normally needs to be shortened.

If resonance is higher than desired, the section is too short. This is why leaving some trimming allowance during construction is useful.

Adjust Resonance

Shorten both sides symmetrically and make small adjustments rather than removing a large amount of wire at once.

  1. Close the first pair of links

    After the highest-frequency section is correct, connect the first extension sections symmetrically.

  2. Measure the next band

    Check the resonant frequency with the antenna installed in its normal configuration.

  3. Adjust the new sections

    Adjust only the newly added outer sections as far as practical.

  4. Continue outward

    Close the next pair of links and continue toward the lowest-frequency band.

  5. Recheck previous bands

    Recheck all previously adjusted bands after tuning is complete.

This inside-to-outside sequence reduces the risk of repeatedly changing sections that affect several lower-band configurations.

Measure SWR with an Antenna Analyzer

An antenna analyzer provides more useful information than an SWR reading alone.

When tuning, check:

  • resonant frequency;
  • resistance, R;
  • reactance, X;
  • impedance;
  • SWR or VSWR/KСВ.

At resonance, reactance is near zero, but resonance alone does not guarantee a perfect 1:1 SWR because the resistive part of the feedpoint impedance may differ from 50 ohms.

Do not tune only for the lowest displayed SWR without considering where the actual resonance occurs and whether feedline common-mode current or the installation itself is influencing the measurement.

Calculation method

Linked Dipole Calculation Formula

The basic calculation begins with the wavelength:

λ = c / f

where:

  • λ = wavelength;
  • c = speed of light;
  • f = frequency.

A free-space half-wave is:

L = c / (2f)

A practical wire dipole is normally shorter than the free-space half-wave, so a correction factor is applied.

Half-Wave Dipole Length

Using frequency in MHz and length in meters:

Total dipole length ≈ 149.896 × K / f(MHz)

where K is the selected correction factor.

For K = 0.95:

Total dipole length ≈ 142.40 / f(MHz)

Each dipole leg is half the total:

Each leg ≈ 71.20 / f(MHz)

The linked dipole calculator applies the same principle to every selected frequency.

Velocity Factor

The correction factor accounts for the fact that a practical resonant conductor does not behave exactly like an ideal free-space half-wave.

If a custom factor is entered, the calculator uses it directly in the starting-length calculation.

Do not confuse this wire correction with the velocity factor of a coaxial transmission line. They describe different propagation conditions and should not automatically be treated as the same value.

Wire and Insulation Correction

Insulation, conductor diameter, construction, nearby materials, and end effects can all shift resonance.

For that reason, two antennas cut to the same nominal frequency can require slightly different final dimensions even when both calculations are mathematically correct.

Use a wire preset for a convenient starting estimate, then verify the assembled antenna with an analyzer.

Inverted V Correction

The geometry of an inverted-V changes the electromagnetic environment of the dipole. Bringing the ends lower and changing the included angle can affect feedpoint impedance, coupling to the ground, and resonance.

There is no single universal shortening percentage that guarantees the correct result for every inverted-V installation. Calculate a reasonable starting length, install the antenna in its normal geometry, and tune it by measurement.

Worked example

40/20/10 m Linked Dipole Example

The following example uses:

  • 40 m: 7.100 MHz
  • 20 m: 14.200 MHz
  • 10 m: 28.400 MHz
  • correction factor: 0.95

Active Dipole Lengths

Band Frequency Full active length Cumulative length per leg
10 m 28.400 MHz 5.01 m / 16.45 ft 2.51 m / 8.23 ft
20 m 14.200 MHz 10.03 m / 32.90 ft 5.01 m / 16.45 ft
40 m 7.100 MHz 20.06 m / 65.80 ft 10.03 m / 32.90 ft

Physical Sections Per Leg

Because each lower-frequency configuration includes all sections closer to the feedpoint, the individual wire sections are calculated by subtracting adjacent cumulative lengths.

Section Approximate length per leg
Inner 10 m section 2.51 m / 8.23 ft
20 m extension 2.51 m / 8.23 ft
40 m extension 5.01 m / 16.45 ft
END — 5.01 m — LINK — 2.51 m — LINK — 2.51 m — FEEDPOINT — 2.51 m — LINK — 2.51 m — LINK — 5.01 m — END

Link Settings

Operating band 10/20 m link pair 20/40 m link pair
10 m OPEN OPEN
20 m CLOSED OPEN
40 m CLOSED CLOSED

These values are calculated starting dimensions. Add any intended trim allowance before cutting and adjust the actual antenna after installation.

Installation comparison

Horizontal Dipole vs Inverted V

Both configurations can use the same linked-dipole principle, but their installation requirements and RF behavior differ.

Characteristic Horizontal dipole Inverted-V
Supports Usually requires elevated support toward both ends plus the center arrangement Can often use one main center mast with lower end anchors
Footprint Greater horizontal width Reduced horizontal span
Feedpoint Center-fed Center-fed at apex
End height Ideally remains elevated Ends slope downward
Feedpoint impedance Depends on height and surroundings Often changes as the included angle becomes smaller
Radiation Depends strongly on height above ground Pattern changes as legs slope downward
Polarization Predominantly determined by conductor orientation and installation Includes fields from sloping conductors
Tuning Final tuning in installed position recommended Final tuning in actual apex geometry especially important

Performance, Impedance and Radiation

A dipole's impedance and radiation pattern are not fixed numbers independent of installation.

They are influenced by:

  • electrical height above ground;
  • apex angle;
  • soil and nearby conductive objects;
  • conductor orientation;
  • feedline interaction;
  • operating frequency;
  • surrounding structures and vegetation.

Changing the antenna height can alter both the elevation pattern and feedpoint impedance. Lower installations generally interact more strongly with the ground, while higher installations can produce different elevation lobes and takeoff angles.

Bandwidth is also affected by conductor characteristics and the antenna's effective Q. A very narrow low-SWR region does not necessarily indicate a better antenna; it simply describes one part of the system's frequency response.

Practical tradeoffs

Linked Dipole Advantages and Limitations

Advantages

Multiband operation One physical dipole can be configured for several HF bands by changing the electrical length.
Resonant band configurations Each selected configuration can be individually trimmed close to resonance instead of relying entirely on an antenna tuner to transform a large mismatch.
Simple construction The antenna can be built from wire, a feedpoint, insulators, links, support line, and suitable feedline components.
Portable-friendly design A linked dipole packs into a small space and can be deployed horizontally or as an inverted-V from a portable mast.
Clear tuning sequence Each band can be adjusted progressively, starting with the shortest inner section and moving outward.

Limitations

Manual band switching Changing bands normally requires opening or closing the appropriate links.
Physical access to links Depending on the installation, the antenna may need to be lowered before switching bands.
Final tuning is still required A calculated conductor length cannot fully predict the influence of real installation height, insulation, soil, vegetation, structures, and feedline interaction.
Several sections increase construction complexity Adding many bands means more insulators, connectors, joints, and opportunities for mechanical or electrical problems.
A tuner does not fix every installation issue An antenna tuner can transform impedance seen by the transceiver, but it does not correct common-mode current, poor mechanical connections, or an incorrectly constructed radiator.
Common questions

Frequently Asked Questions

What is a linked dipole antenna?

A linked dipole is a center-fed dipole divided into sections that can be electrically connected or disconnected. Changing the links changes the active conductor length, allowing one antenna to operate resonantly on several bands.

How do you calculate a linked dipole?

Calculate the required half-wave dipole length for every selected frequency, divide each total by two to obtain the cumulative length of one leg, then subtract adjacent cumulative lengths to find the individual sections between links.

How long is a 40 meter dipole?

It depends on operating frequency and wire correction. With a 0.95 correction factor, a dipole for 7.100 MHz has a calculated starting length of about 20.06 m, or 65.80 ft.

How long is each leg of a 40m dipole?

At 7.100 MHz with a 0.95 correction factor, each leg is approximately 10.03 m or 32.90 ft before final field tuning.

Can a linked dipole be installed as an inverted V?

Yes. A linked dipole can be supported as an inverted-V, provided the links, insulators, and feedpoint remain mechanically secure and the antenna is tuned in that installation geometry.

What angle should an inverted V antenna have?

There is no single angle that is ideal for every installation. The apex angle affects footprint, end height, feedpoint impedance, and radiation behavior, so choose an angle that fits the support geometry and confirm the result by measurement.

Does a linked dipole need a tuner?

A correctly adjusted linked dipole may provide a usable match on its designed frequencies without requiring a tuner, but the actual SWR depends on installation and feedpoint impedance. A tuner can still be useful when operating away from the tuned frequencies.

Does a linked dipole need a balun?

A 1:1 current balun or common-mode choke is commonly useful because a dipole is balanced while coax is unbalanced. It helps prevent the outside of the coax shield from becoming an unintended part of the antenna.

Which section should I tune first?

Tune the shortest inner section first. This is normally the highest-frequency band. Then close the next links and work outward toward progressively lower frequencies.

How much extra wire should I leave for tuning?

Leave enough extra conductor to permit final adjustment rather than cutting directly to an irreversible minimum length. The appropriate allowance depends on the construction and wire system, so the calculator should expose a configurable trim allowance rather than assume one universal value.

Does insulated wire change dipole length?

Yes, insulation can change the electrical behavior of the conductor and therefore the physical length required for resonance. Use a suitable starting correction factor and verify the finished antenna with an analyzer.

Why is my calculated dipole resonant at the wrong frequency?

Common reasons include wire properties, insulation, installation height, inverted-V angle, nearby objects, ground interaction, inaccurate dimensions, connector effects, and common-mode current on the feedline.

What SWR should a resonant dipole have?

Resonance means the reactive component of impedance is near zero; it does not automatically mean a perfect 1:1 SWR. The measured SWR also depends on how the resistive feedpoint impedance compares with the feedline's characteristic impedance.

Can I use one linked dipole for 40, 20 and 10 meters?

Yes. A 40/20/10 m linked dipole can use the 10 m section at the center, a 20 m extension outside the first links, and a 40 m extension outside the second pair of links.

Methodology

Calculation Methodology and Accuracy

This calculator is intended to provide practical starting dimensions, not a claim of millimeter-level prediction of the finished antenna.

The calculation process is:

  1. Convert frequency

    Convert the selected frequency into a free-space wavelength.

  2. Calculate the half wavelength

    Calculate one half wavelength.

  3. Apply the correction factor

    Apply the selected wire correction factor.

  4. Calculate each leg

    Divide the full dipole into two equal legs.

  5. Calculate cumulative linked lengths

    For a linked dipole, calculate the cumulative leg length for every frequency.

  6. Calculate individual sections

    Subtract adjacent cumulative lengths to determine each individual section.

  7. Mirror the antenna

    Mirror all sections on the opposite side of the feedpoint.

  8. Add trim allowance

    Add the user-selected trimming allowance where requested.

  9. Calculate inverted-V geometry

    For an inverted-V, calculate the installation geometry from leg length and apex angle.

Actual resonance can shift because of:

  • insulation;
  • conductor diameter;
  • link and connector construction;
  • feedpoint hardware;
  • antenna height;
  • inverted-V angle;
  • ground conditions;
  • vegetation and nearby structures;
  • feedline routing;
  • common-mode current;
  • measurement environment.

For final adjustment, install the antenna in its normal configuration and use an antenna analyzer to check resonance, resistance, reactance, impedance, and SWR. Tune the highest-frequency section first and continue outward.

Related Antenna Calculators

Important: Calculated dimensions are starting values. Always verify the finished antenna in its intended installation before treating a calculated value as the final resonant length.