# What is the peak voltage at the tips of a dipole antenna?

What is the peak voltage present at the very end tips of half-wave dipole antenna in free space, and how might this peak voltage relate to transmitter type, transmitter power, RF frequency vs. antenna half-wave frequency mismatch, feed line, SWR, wire diameter, and etc.

I'm going to approach this a little differently starting from roughly the same place. Here I am going to use a resonant $\lambda$/2 20m dipole driven by 100 W as the model.

Let's compute the current at the feed point of a dipole at resonance, this is found with the input power (100 watts) and the feed point impedance; which for our dipole is assumed to be the theoretical 73 $\Omega$ :

$$I = \left(\frac{W}{R}\right)^{\frac{1}{2}} = \left(\frac{100 \mathrm W}{73 \Omega}\right)^{\frac{1}{2}} = 1.17 \: \text{amps (RMS)}$$

Therefore the driving voltage can be calulated with Ohm's Law:

$$V_\text{feed} = I \cdot R = 1.17 \mathrm A_\text{RMS} \cdot 73 \Omega = 85.44 \:\mathrm V_\text{RMS}$$ (unmodulated signal)

The voltage at the end of the dipole would require us to calculate the Q and solve the following:

$$V_\text{end} = \frac{Q\:V_\text{feed}}{2}$$

Trying to minimize the hand-waving, we can use some approximations from transmission line theory to give us the Q. (See Edmund Laport's Radio Antenna Engineering for a complete (and math heavy) explanation) To do this we need the characteristic impedance of the dipole (considered as a transmission line). That is given by:

$$Z_{0} = 276 \cdot \log_{10}\frac{l}{p} = 972.31 \Omega$$

Where $l$ is the total length of the dipole and $p$ is the radius of the conductor (all in the same units). I am going to ignore calculating the exact length here, we know it's approximately 5% shorter than the real wavelength to make up for velocity factor and end effects. This next bit leans on transmission line theory and can turn into a bag of snakes, if you want to know more about where these equations come from, check the reference quoted above. $Q$ here is the ratio of the voltage of the direct wave and the reflected wave:

$$Q = \frac{1+m}{1-m}$$

and $m$ is calculated from the feed point impedance $R$ and the characteristic impedance $Z_0$:

$$m = \frac{Z_0-R}{Z_0+R}$$

When I calculate $\ Z_0$, I am going to assume our dipole is made with 3mm wire. Now to crank through the numbers:

$$m = \frac{972\Omega-73\Omega}{972\Omega+73\Omega} = .86$$

$$Q = \frac{1+.86}{1-.86} = 13.29$$

Now we can solve for $V_\text{end}$:

$$V_\text{end} = \frac{(13.29 \cdot 85.44 \mathrm V)}{2} = 568 \:\mathrm V_\text{RMS}$$

Again, this is the RMS voltage we should convert to peak voltage:

$$568 \:\mathrm V_\text{RMS} \cdot \sqrt{2} = \pm 804 \:\mathrm V_\text{peak}$$

This is all for 100W, if we instead plug 1500W into the above math, we come up with

$$4397 \:\mathrm V_\text{RMS} \:\text{or} \: \pm 6200 \:\mathrm V_\text{peak}$$

That's a pretty hefty jolt. So getting back to the OP's other questions, the input power has a substantial effect on the voltage. The rest of the factors are all the same as for maximizing antenna efficiency (resonance, conductor size, etc.)

EDIT: Most of the above equations come from the section on Circuital Design in the reference listed above. The book is more math heavy than typical amateur radio references, but not as bad as some of the more modern engineering texts. It's slow going, but a worthwhile read.

• An interesting consequence of this which I had not previously considered: a thicker antenna will have a lower peak voltage. (And also: wider bandwidth, lower resistive losses. Overall a win.) Feb 12, 2014 at 16:07
• Would the reported computation be equivalent to this (since you already computed the characteristic impedance) 972.31 Ohm * 1.17 Amps / 2 = 568 V (rms) ? Mar 26, 2018 at 22:56
• In running through the numbers, it appears you used the wire size diameter, rather than the radius as called for in the formulas cited. Wire size of 3mm would have a radius of .0015, but the calculation appears to use diameter of 3mm (.003m) or approximately 10AWG wire. Or did you mean to say that you used 6mm diameter wire? At 1500W, then, the V-pk is closer to ±6881V-pk at 14.2Mhz, for example, versus the ±6200 calculated. Can you comment on how this method applies to the voltage(s) at the end of an elevated Ground Plane (tip of radiator and ends of 4x radials)?
– K1VF
Nov 11, 2018 at 15:47
• Z0=276⋅log10lp=972.31Ω Where does 276 come from in this formula? And will this value (276) change in a 50 ohm dipole antenna? Please help me for my calculate tnx. Met Nov 4, 2020 at 12:20
• @HAMRADIO Apparently I slept since I wrote this post. I have been out of radio for some years. Looking back through these equations, I can see why you are confused about the number, but I can't think of it myself, it must have come from the textbook. Nov 5, 2020 at 18:35

It's really hard to say, because it depends on so many things. Analyzing the antenna in free space simplifies some things, but we'd still have to consider the exact geometry of the antenna (How thick are the wires? Are they bent at all?) and the material from which they are made (any resistance will decrease the Q factor of the antenna, reducing the peak voltage).

However, if you look to analysis of end-fed dipoles, you can find that it's been determined empirically and by modeling that the impedance at the end of a real half-wave dipole is somewhere between 1800 to 5000 ohms.

Knowing this, we can calculate what the voltage is for a given power into the antenna. If we are putting 100W into the antenna, and we figure the impedance at the ends is 4000 ohms, then:

\begin{align} P &= V^2/R \\ 100\mathrm W &= V^2 / 4000\Omega \\ \sqrt{100\mathrm W \cdot 4000 \Omega} &= V \\ V &\approx 632 \mathrm V \end{align}

This is an RMS value. Knowing that our transmission is approximately sinusoidal, then the peak voltage is something like:

$$632 \cdot \sqrt{2} = \pm 894 \mathrm V$$

From the above equations, we can see that power is proportional to the square of voltage:

$$P \propto V^2$$

This is the power delivered to the antenna. Transmitter type and the match to the antenna (SWR) are relevant only to the extent that they change the power delivered to the antenna.

This is all assuming that the antenna is operated at resonance. As the frequency moves away from resonance, the peak voltage decreases. The reason why is simple: this high voltage is attainable because each cycle reinforces the previous. If you take a limiting case where the antenna is operated at DC, the voltage at the ends is equal to the voltage at the feedpoint, because there is no resonance to reinforce the voltage at the ends.

For those of you with EZNEC or some other antenna modeling software, there is a way to answer this question using EZNEC. Model a 1/4WL stub in free space taking care not to violate any geometry checks. Put a 100w source at one end of the stub and a 10 megohm load at the other end of the stub. Adjust the stub length and user defined wire loss to obtain the resistive feedpoint impedance of a dipole looking into the stub. Then display the load data. It will tell you the voltage at the end of a dipole. I set my 4 MHz stub for 70 ohms and got 879 volts across the 10 megohm load resistor. The additional user defined wire loss is equivalent to the power lost from the dipole through radiation.

• Cecil! It's good to see you here! Gentlemen, welcome another BSEE! :-) Nov 12, 2018 at 0:09

The current at the ends of a half-wave dipole vanishes, so the answer to your question must be that the peak voltage at the ends is zero.

The current distribution along a half-wave dipole is a standing wave, expressed mathematically by $$I(z) = I_0 \cos(2\pi f t)\cos(kz)$$

where $$k = 2\pi/\lambda$$, $$f$$ is the carrier frequency, $$\lambda$$ is the wavelength ($$= c/f$$), and $$z=0$$ is the feedpoint at the center. The voltage is related to the current by ohms's law: $$V(z) = I(z)\cdot R_{rad}$$ where $$R_{rad}$$ is the radiation resistance of the antenna. In the case of a half-wave dipole, $$R_{rad}\approx 73.1\Omega$$.

The ends are at $$z=\pm \lambda/4$$, where $$kz = \pm\frac{2\pi}{\lambda}\cdot\frac{\lambda}{4} = \pm \frac{\pi}{2}$$ so that $$\cos(kz)$$ at the ends is zero. Hence the current and the voltage must both be zero at the ends.

All of the above assumes a perfectly matched ideal half-wave dipole with 1:1 SWR and perfect conductors. Under other than ideal conditions several things can happen.

If, for example, the antenna is mismatched, then there will no longer be a standing wave at the end of the antenna and the current distribution expression above is no longer valid. The peak of the current might shift slowly back and forth between the two ends, in which case the peak current at the end might be $$I_0$$ in the worst case. Another answer derives this for you as a function of transmit parameters.

Another effect might be loss in the antenna wire, which could take place when the transmitter is trying to push a lot of power through a thin wire. Loss, and hence heating would result, but barring a bad mismatch the current would also vanish at the ends in this case.

Still another factor might be the bandwidth of the signal. The antenna is only resonant - i.e. a half-wave length - at one specific carrier frequency $$f$$, where $$l = \frac{1}{2}\frac{c}{f}$$ At the band edges, the antenna's length in terms of signal wavelength is $$\frac{l}{\lambda_\pm} = \frac{1}{2}\left(1 \pm \frac{B}{2f}\right)$$ where $$B$$ is the signal bandwidth. Off resonance we again have a semi-traveling wave where the peak current at the tips doesn't vanish. It's magnitude depends on how much energy is in the signal off the carrier frequency.