I have seen the following formulas for calculating half and quarter wavelength antennas:

Formula for $\frac{1}{2}$-wavelength antenna (in free space):

\begin{equation} \mathrm{Length~(feet)} = \frac{492}{f_{MHz}} \end{equation}

Or is it...

\begin{equation} \mathrm{Length~(feet)} = \frac{468}{f_{MHz}} \end{equation}

Formula for $\frac{1}{4}$-wavelength antenna (in free space):

\begin{equation} \mathrm{Length~(feet)} = \frac{246}{f_{MHz}} \end{equation}

Or is it...

\begin{equation} \mathrm{Length~(feet)} = \frac{234}{f_{MHz}} \end{equation}

Or is it none of the above? I believe the US FCC Technician class exam requires the use of 468/f. Are any of these equations helpful in calculating antenna length in reality, or is this only in theory for the exam?

What additional factors should be taken into account, if any? What would be a better equation if none of the above?

  • 3
    $\begingroup$ For dipoles and loops, in real life you cut it long and use an antenna analyzer as you trim it down. $\endgroup$
    – Paul
    Commented Oct 24, 2013 at 21:30
  • $\begingroup$ @SDsolar - VF of copper wire is more like 95% of free space $\endgroup$
    – mike65535
    Commented May 19, 2018 at 12:06

6 Answers 6


The $492/f$ formula is for an ideal antenna in free space, the $468/f$ is an estimate for real antennas at a reasonable height over ground.

The $492/f$ formula is a conversion from metric units to English units for the fundamental frequency and wavelength ($\lambda$) formula. $c = 3\times 10^8_{m/s}$ (the velocity of light) and $f =$ frequency --

\begin{equation} \lambda = \frac{c}{f} \end{equation}

This gives the length of a full wavelength in meters. This formula is correct if the conductor is infinitely thin and other objects are infinitely far away from the antenna.

The length of a real, installed antenna is affected by the diameter of the conductor (not a big effect for wire antennas) and the height above ground (a big effect). Capacitance to ground electrically shortens the antenna, so less wire is needed for resonance.

$468/f$ is a good estimate for wire antennas at HF less than a wavelength above ground. This is an empirical formula, so there is no mathematical derivation. The $468/f$ formula was first published in the 1929 ARRL Handbook. It is probably based on experience with 40m and 80m antennas at heights of 1/4 to 1/8 wavelength above ground, since those were common antennas at the time.

A November 2009 QST article by Ward Silver, N0AX, measured a 20m dipole at heights from 1/8 to 2 wavelengths and found the length varied from $466/f$ to $481/f$ depending on height. He recommends starting with a wire length of $490/f$ and expecting to shorten the antenna to resonance.

Most wire antennas need length adjustment for resonance after installation, because of the capacitance to nearby structures or trees, or local ground conductivity. It is much easier to shorten an antenna than to lengthen it, so it is a good idea to cut the antenna wire a little long.

For more on this publication history of this formula, see this article by N0AX.

For more information about wire antennas, I would start with Chapter 21 of the ARRL Handbook. For details, read the ARRL Antenna Book.


For someone who knows how to convert between inches, feet, and meters, it's really quite simple. You only really need to know one formula to do it all, and that formula is $300=f\times wavelength$. If you find the wavelength for the given frequency, then just find the type of antenna (quarter-wave), take the appropriate fraction of the wavelength, and convert said quantity to the appropriate units. For example, the wavelength for a 146 MHz signal is 2.05 m, multiply by 39 and you have 80 inches. If you want a quarter wave whip, then your antenna is 20 inches long.

As to where this applies after the test, it does apply, but there is one huge catch. The antenna needs to have the provided wavelengths electrically, not physically. What does that mean? Basically, there's a quantity known as Velocity Factor which takes into account how fast the waves move in the metal. However, most metals have a permittivity of about 1, making the electric distance equal to the physical distance. Some non-metal antenna materials could be different, however, so be warned. Also, cable is different, etc. Essentially, if the velocity factor of an antenna is 2, then an antenna could be made with half of the length and still be resonant. However, as the velocity factor for most metals is 1, and there are other reasons to use metal as antenna building material, this isn't usually a significant factor. It does make a small difference in certain types of phased antennas, however.

As to your specific question, the half-wave formula is $(3.28/2)(300/f)$, or $492/f$, and the quarter wave is similarly $(3.28/4)(300/f)$ or $246/f$. This applies if the velocity factor is 1, which only holds true if the antenna is far away from conductive surfaces, including the ground. The distance required is at least 1 wavelength away typically.

  • $\begingroup$ I can tell you know what you're talking about. But I'm not following entirely. Can you spell it out into some sort of equation? $\endgroup$
    – Dan
    Commented Oct 24, 2013 at 15:49
  • $\begingroup$ @Dan: Hopefully that's a bit better. $\endgroup$ Commented Oct 24, 2013 at 15:54
  • 1
    $\begingroup$ Velocity factor is not the best model for this. We talk about velocity factor as a characteristic of the transmission line itself. A dipole over ground is shortened by stray capacitance to the environment rather than by a characteristic of the wire. This shortening can be increased with capacitive loading at the ends, and you commonly see this in vertical dipoles for HF and sometimes as a "capacity hat" for a mobile HF antenna or a vertical for 160m. $\endgroup$ Commented Oct 24, 2013 at 18:59
  • 1
    $\begingroup$ Neither answer currently addresses why there are two formulas out there and explain where the other came from - which is what I am looking for. Please demonstrate which is better mathematically, don't just cite ARRL or another source. $\endgroup$
    – Dan
    Commented Oct 24, 2013 at 19:02
  • $\begingroup$ @Dan: Good point, answered your specific question now. $\endgroup$ Commented Oct 24, 2013 at 19:11


  • $c$ = velocity of propogation = speed of light (299,792,458 meters/second)
  • $f$ = frequency
  • $\lambda $ = wavelength


The basic formula for calculating wavelength is:

\begin{equation} \lambda = \frac{c}{f} \end{equation}

To make the math simpler, frequency ($f$) is expressed in megahertz (MHz) and the velocity of propogation in free space ($c$) for frequencies above 30 MHz is expressed as and rounded to 300 megameters (Mm). This will return a wavelength ($\lambda$) in meters. So for 1 wavelength above 30 MHz:

\begin{equation} \lambda_{m} = \frac{300}{f_{MHz}} \end{equation}

However, when $f < 30_{MHz}$, the velocity of propogation ($c$) is expressed as and rounded to 286 Mm because

"[e]lectrical wave propagation in wire is about 95% to 97% the speed of light. Since wavelength is most commonly used for building antennas which involve conducting the wave from air into the wire and vice versa, the calculation is adjusted assuming the slower propagation in an unshielded conductor.

"However, this 3% to 5% discrepancy is small enough at frequencies above 30 MHz that it is usually ignored for simplicity, and 300 Mm is used instead" (Adam Davis, KD8OAS).

When $f < 30_{MHz}$ the discrepancy becomes more significant and the adjusted value, approximately 95% of 300 Mm, is used instead, which is approximately 286Mm (which would actually be $0.95\overline{3}$). This results in the following formula for 1 wavelength below 30 MHz:

\begin{equation} \lambda_{m} = \frac{286}{f_{MHz}} \end{equation}

To convert this into feet, multiply $c$ by 3.28084, which results in the following formula for receiving an answer in feet when $f > 30_{MHz}$:

\begin{equation} \lambda_{ft} = \frac{(3.28084)300}{f_{MHz}} = \frac{984.252}{f_{MHz}} \end{equation}

This is rounded down to $984/f$ for the sake of simplicity. However, recall that when $f < 30_{MHz}$, the velocity of propogation ($c$) is expressed as and rounded to 286 Mm. Applying this formula results in the following for converting this into feet below 30 MHz:

\begin{equation} \lambda_{ft} = \frac{(3.28084)286}{f_{MHz}} = \frac{938.32024}{f_{MHz}} \end{equation}

This is also rounded down to $938/f$ for the sake of simplicity.

Calculating for half and quarter waves is just a manner of of dividing $c/2$ or $c/4$, respectively. So we end up with the following calculation for calculating the length of half wave antennas in feet when $f > 30_{MHz}$:

\begin{equation} \lambda_{ft} = \frac{(3.28084)(300/2)}{f_{MHz}} = \frac{492.126}{f_{MHz}} \end{equation}

When calculating the length of half wave antennas in feet where $f < 30_{MHz}$, we have the following formula:

\begin{equation} \lambda_{ft} = \frac{(3.28084)(286/2)}{f_{MHz}} = \frac{469.16012}{f_{MHz}} \end{equation}

But this is generally expressed as $468/f$, not as 469. Why is this? First of all, remember that the velocity factor is approximately 95-97% of the speed of light, so adjusting this value results in slightly different results. Also, whether we use the adjusted value of $c$ when $f < 30_{MHz}$ (286 Mm) or apply the velocity factor directly to $c$ will slightly alter our result. So for instance, the following calculation will get us closer to $468/f$:

\begin{equation} \lambda_{ft} = \frac{(3.28084)((300/2)(0.95))}{f_{MHz}} = \frac{467.5197}{f_{MHz}} \end{equation}

This would round up easily to $468/f$ when $f < 30_{MHz}$, and it is slightly more accurate.

This shows why there are different equations and when each should be used.

  • 2
    $\begingroup$ I downvoted this because it is not the right model for analyzing antennas. We use velocity factor for transmission lines, not for antennas. Velocity factor is based on the distributed capacitance, distributed inductance, and dielectric constant of the transmission line. For an antenna, the capacitance to ground is not evenly distributed, so these models are not a good choice. For example, the end capacitance effect is larger for an inverted vee. Also, assuming an unsupported choice for velocity factor does not make this based on physics, even though it makes the numbers come out almost right. $\endgroup$ Commented Oct 29, 2013 at 21:29
  • $\begingroup$ @WalterUnderwoodK6WRU interesting. Do you have any additional references where I could read more about this? I'm trying to learn this stuff with the goal of being able to calculate this kind of stuff. $\endgroup$
    – Dan
    Commented Oct 29, 2013 at 21:37
  • $\begingroup$ The velocity factor is what most of the above keep missing from the equations, and the difference between 492 and 468. Looks like Dan was the only one who got it. The velocity factor of 0.951 was that of solid copper back in 1929, when this conversion was first (that I know of) published. $\endgroup$
    – user5165
    Commented Aug 18, 2015 at 3:08
  • $\begingroup$ @nojiratz Velocity factor is a dielectric effect in a transmission line, it's not applicable to a bare conductor. True, a resonant dipole is less than lambda/2, it's more like 0.48 for very thin wire, and 0.45 for thicker wire. This applies equally to any conductor, not just copper. $\endgroup$
    – tomnexus
    Commented Aug 18, 2015 at 19:58
  • $\begingroup$ I learned the adjustment from $\lambda$ to the electrical length is referred to as a shortening factor to allow for the diameter to length ratio of the conductor and any end effect caused by loading from wrapping wire around insulators, etc. This shortening factor was determined experimentally. I also learned to apply it when $f < 30 MHz$ or so. The takeaway is that the electrical length is an approximation. So while velocity factor is probably the wrong term here, the approximation in SI units seems correct. $\endgroup$
    – user21417
    Commented Mar 21, 2022 at 15:07

Thanks for the posting everyone! For licence test I took this approach after reading everyone's post & searching though all the technical details you posted.

  1. Convert Frequency to wavelength in meters. 300 ÷ frequency.
  2. Multiplying 39 × wavelength in meters = inches of full Antenna length.
  3. Divide inches by 2 for 1/2 wave.
  4. Divide 1/2 wave by 2 for 1/4 wave.

Example. 146Mhz 300÷146=2.05 meters
2.05×39= 79.95 inches full length in inches.
79.95÷2= 39.95 inches 1/2 wave length in inches.
39.95÷2= 19.985 inches 1/4 wave length in inches.
Answer on test is 19.

Example 6m. Meters already given.
6×39= 234 inches full wave length in inches.
234÷2= 117 inches 1/2 wave length in inches.
Answer on test is 112. Which is rounded answer.

You only have to remember find wavelength in meters & multiply 39 then find antenna wavelength in inches. Please advise me if these calculation are in error or any other errors. 73's


I always use the 468 formula and have for the past 30 years and ALWAYS had a perfect SWR and matched antenna. I have made over 200 dipoles and I have NEVER had to trim to get a perfect antenna. I also have NEVER made an antenna too short or too long!


Need to get a few things out of the way to understand why some things are.

  1. Velocity Factor - speed of a electromagnetic (EM) wave through ANY material.
  2. Frequency - Speed in Hz of a (EM) wave. 20Hz to 20kHz is Audio, 100kHz and above is considered Radio until nanometers then it's visible then on to other types. We are referring to RF.
  3. Antenna - item for receiving and transmitting an electromagnetic wave.
  4. Transmission Line/Coax - item to convey electromagnetic wave to/from antenna and radio.
  5. Skin Effect - the tendency of (EM) wave to migrate to the outside edge of a conductor.

A. Velocity factor in antenna building does NOT matter unless

  1. You are using coax or transmission line as part or all of the antenna.
  2. You are calculating an antenna for use under 50 MHz. Only then does the velocity factor of the line need be known. And usually it is LESS than 1. This factors into the size of the antenna as well. Very important to those co-linear antennas everyone wants to build for the gain.

B. Personally, use the L(feet)=234/f in MHz for 1/4 wave and 468/f in MHz for 1/2 wave antennas. This works for all antennas used to about 2 GHz, After that a gnat hair changes the tuned frequency.

C. An antenna that is broadband is NOT going to have a large amount of gain, and is better suited to receiving, i.e., scanner antennas.

D. An antenna that is narrow-banded can exhibit a large amount of gain, but operate in a narrower bandwidth. These are best suited for repeater antennas, as the repeater transmits on ONE frequency. Some can be engineered with electrical down-tilt to increase coverage below the horizon of the antenna.

E. An antenna uses tubing for two purposes, the first is fairly obvious, weight. A tube is much lighter than a solid rod of the same length and diameter. Tubing is usually the choice when building any antenna that has multiple elements usually a beam antenna and used in large single- and multi-band verticals. Wire for antennas can be found that uses a stronger inner core coated with a variety of materials to make it conduct better on the outside circumference making it ideally suited for long wire use.


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