Why is a 1/4 wavelength antenna limited to 1/4 wavelength length?

In summary: The currents will flow towards the ground plane and reflect off of it in all directions. These currents will be in phase with the electric field that is radiated by the vertical radiator. The currents will also be out of phase with the electric field that is radiated by the horizontal radiator. The currents that are in phase with the vertical electric field will be amplified and the currents that are out of phase will be canceled out. This causes the antenna to act like a dipole. But if you move the antenna away from the ground plane, the currents that are in phase with the horizontal electric field will start to dominate and the antenna will start to act like a monopole.
  • #1
d.arbitman
101
4
Why does a 1/4 wavelength antenna have to be 1/4 wavelength? What property of the wave is responsible for this restriction?
I've been trying to understand how a 1/4 wavelength antenna works and the best explanation, relatively speaking, was on the following website, http://www.sm0vpo.com/antennas/anten.htm .

It still doesn't make any sense. Maybe if I could understand how a 1/4 wavelength antenna works, I could figure out why there is a restriction on the length.
 
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  • #2
Do you understand how a dipole works? Roughly by making an antenna a half wavelength you minimize reflections and reactive components such that maximum power transfer occurs when it is matched properly. (an oversimplification)

A quarter wave kind of uses ground (well, a reflection) for the other half of the dipole.

The wikipedia dipole article describes it pretty well.

Actually, the article you pointed to describes it well too. If the length is wrong the reflections are not additive. You can go to longer multiples if you want.
 
  • #3
meBigGuy said:
Do you understand how a dipole works? Roughly by making an antenna a half wavelength you minimize reflections and reactive components such that maximum power transfer occurs when it is matched properly. (an oversimplification)

Yes, I presume I understand since all of the videos I watched and articles I read make sense.

meBigGuy said:
A quarter wave kind of uses ground (well, a reflection) for the other half of the dipole.

I don't understand how the reflected portion of the signal constitutes the other 1/4 length of a dipole.
 
  • #4
Realize that only the 1/4 wave section actually radiates. The reflection only serves to make the 1/4 wave antenna non-reactive (not capacitive or inductive) and an efficient radiator.

The 1/4 wave antenna depends on the ground plane being large enough to actually cause physical reflections of the 1/4 wave conductor. If there is no ground plane it does not work. The article you referenced explains it pretty well. ("The diameter of the tin-plate is assumed to be more than 1/2-wave"). In the wikipedia dipole antenna article they are a little more technical about the quarter wave monopole. This link addresses it also with a bit about the effect of a small ground plane http://www.antenna-theory.com/antennas/monopole.php

But none of this is a near-field analysis of how the reflections work.

If you really want to understand you need to work up to this I suppose (I'm not there) http://www.ece.rutgers.edu/~orfanidi/ewa/ch14.pdf. What you ask may well be covered in that book somewhere. http://www.ece.rutgers.edu/~orfanidi/ewa/

A google search for "near field antenna analysis monopole" yielded a lot of stuff.

http://ece.wpi.edu/mom/chapter4.pdf seems to get pretty deep.
 
  • #5
I'll be reading those. I wasn't sure if the article for which I provided a link was talking about a physical reflection, like a signal bouncing off of a wall or an electrical signal in a conductive medium at a discontinuity (e.g. what happens when you have impedance mismatch). I didn't know what terms to search for. Thank you.
 
  • #6
I've read through those but still don't intuitively understand what's happening in a monopole antenna.
 
  • #7
All I can say is that the reflection causes the monopole section to act like there is another monopole section which it interacts with in much the same ways as it would it were a dipole rather than a relection.

If you think of the combined signal and reflection at an arbitrary single point on a monopole, it is the same as the signal and its symmetrical point on a dipole. The distance from any point on the monopole to the reflector and back is the same as the distance to the symmetrical point on the dipole, so the phases are the same in terms of how the signals interact. That causes it to act the same as a dipole. But you really have to fully understand the dipole to fully understand that (remeber the dipole halves are fed out of phase).
 
  • #8
A wave traveling along a half wavelength and reflecting from the cut end will get back in time with the next cycle. That is the resonant half dipole situation.

Now get a drinking straw, assume it is half a wavelength long, cut it in half and place one end against a mirror. It will now look the same length as it did before you cut it. That is why a quarter wave antenna over a ground plane is resonant.

The antenna length can be different to a half or a quarter wavelength but there will have to be some phase matching network to bring it to resonance.
 
  • #9
d.arbitman said:
I've read through those but still don't intuitively understand what's happening in a monopole antenna.

One way to look at is is to consider the currents flowing in the ground due to the fields from the vertical radiator. An antenna mounted at a height above a ground plane will produce currents in the plane which will produce a reflection of the antenna (exactly the same as the currents in a shiny metal reflector will cause a reflection and an optical image which appears to be the same distance 'behind' the reflector as the object. (Mounting an antenna at great height will give you another, virtual, antenna below ground and increase the gain of the antenna in the forward direction: so called Height Gain) The details of the current distribution over the plane are complicated and correspond to the same Maths that are used to describe diffraction - which is another way to 'construct' the visible image.
For a quarter wave dipole, there are Earth currents flowing, induced by the vertical bit and these generate a wave which is the same as would exist if the Earth plane were replaced by the other half of the dipole.
Don't lose sleep if you cannot do the sums for this - the essential thing is to appreciate that reflections in conductors are due to (or can be explained in terms of) induced currents.
 
  • #10
sophiecentaur said:
One way to look at is is to consider the currents flowing in the ground due to the fields from the vertical radiator. An antenna mounted at a height above a ground plane will produce currents in the plane which will produce a reflection of the antenna (exactly the same as the currents in a shiny metal reflector will cause a reflection and an optical image which appears to be the same distance 'behind' the reflector as the object. (Mounting an antenna at great height will give you another, virtual, antenna below ground and increase the gain of the antenna in the forward direction: so called Height Gain) The details of the current distribution over the plane are complicated and correspond to the same Maths that are used to describe diffraction - which is another way to 'construct' the visible image.
For a quarter wave dipole, there are Earth currents flowing, induced by the vertical bit and these generate a wave which is the same as would exist if the Earth plane were replaced by the other half of the dipole.
Don't lose sleep if you cannot do the sums for this - the essential thing is to appreciate that reflections in conductors are due to (or can be explained in terms of) induced currents.

It's very hard to picture that considering the 1/4 wavelength antenna has currents running vertically whereas the ground plane would have ground currents running horizontally due to the orthogonal relationship between the two. I have read about the analogy of looking at "half" of an object in the mirror and it would resemble a whole, however I'm drawing a blank at the science behind it. I don't see how the ground plane mimics the behavior of the other 1/4 wavelength antenna.
 
  • #11
The reflected signal from the ground plane is exactly the same as what a radiator would generate. The monopole cannot tell the difference. It cannot tell whether it is talking to another monopole or its own reflection. If you want to fully understand it you will have to trace paths and see it is the same. Look at the EM waves that cross over the center plane for a dipole (a plane orthogonol to the antenna at the feed) and see they are the same as a reflected wave at that plane.
 
  • #12
http://www.aa5tb.com/dipole01.gif

If you put a reflector in the middle of that antenna (and fed it correctly) the current and voltage patterns would look identical. If you want the mathematical proof or derivation of that, I can't help you other than the reference material I already posted.
 
  • #13
meBigGuy said:
http://www.aa5tb.com/dipole01.gif

If you put a reflector in the middle of that antenna (and fed it correctly) the current and voltage patterns would look identical. If you want the mathematical proof or derivation of that, I can't help you other than the reference material I already posted.

I've seen that graphical illustration of a dipole and I understand it. I just don't understand how the monopole antenna has the same current/voltage curve. What happens at the ground plane that causes the same behavior?
 
  • #14
d.arbitman said:
It's very hard to picture that considering the 1/4 wavelength antenna has currents running vertically whereas the ground plane would have ground currents running horizontally due to the orthogonal relationship between the two. I have read about the analogy of looking at "half" of an object in the mirror and it would resemble a whole, however I'm drawing a blank at the science behind it. I don't see how the ground plane mimics the behavior of the other 1/4 wavelength antenna.

Two ways of thinking about this problem, which may help. (It could be a visualisation matter). I remember 'feeling' that the E fields everywhere around the monopole must be vertical but they are not.
1. Remember. If you are looking at the antenna from anywhere other than right down on the plane of the Earth plane, you will see a component of both the vertical currents in the monopole and the horizontal currents in the Earth plane.
2. Take a small element of the vertical wire. This is a 'short' radiator and the E field will only be vertical in the horizontal direction. The E field lines will go out of the top of the element, round and into the bottom of the element (i.e. not all vertical). So the elemental E fields will actually have a component in the plane of the Earth plane if they have originated from anywhere above the plane. Hence, you can get an induced a current which is at right angles to the direction of the originating current.
 
  • #15
sophiecentaur said:
Two ways of thinking about this problem, which may help. (It could be a visualisation matter). I remember 'feeling' that the E fields everywhere around the monopole must be vertical but they are not.
1. Remember. If you are looking at the antenna from anywhere other than right down on the plane of the Earth plane, you will see a component of both the vertical currents in the monopole and the horizontal currents in the Earth plane.
2. Take a small element of the vertical wire. This is a 'short' radiator and the E field will only be vertical in the horizontal direction. The E field lines will go out of the top of the element, round and into the bottom of the element (i.e. not all vertical). So the elemental E fields will actually have a component in the plane of the Earth plane if they have originated from anywhere above the plane. Hence, you can get an induced a current which is at right angles to the direction of the originating current.

So if we suppose that the ground plane is actually parallel to the ground and the monopole itself is vertically oriented, then the E field that is due to the monopole mainly looks like it does in the following picture: http://web.ncf.ca/ch865/graphics/EFldChargedCylinder.jpeg i.e. the E field is "parallel" to the ground plane. Because the E field is "parallel" to the ground plane it will induce current in the ground plane and they will be in phase with the current in the antenna itself. Is my analysis correct?

Why does the ground plane have to exist? Why wouldn't the antenna radiate (at the same frequency) if there was no ground plane?
 
  • #16
Sorry, that picture is hard to understand. There is no E field actually at the plane - which is why the currents are induced (boundary conditions apply), any waves arriving just have to be reflected. The induced E fields are symmetrical in direction about the vertical (laws of reflection - in optics - same thing).
The ground plane doesn't "have to exist" but its presence causes two things. It gets the feed point impedance to half the value of the dipole. It also defines a path for currents in the other half (the screen or other one of the pair) of the feeder to flow into. If you just stick a coax in the air, with a length of the inner sticking, out every Amp that flows in the exposed bit needs to flow down the outside of the screen. This gives an uncertain impedance and an uncertain radiation pattern. (Kirchoff 1 applies at the drive point, as ever)
And of course, actually, the other reason for currents flowing in the Earth plane is that the Earth current from the feeder has to flow somewhere.
 
  • #17
sophiecentaur said:
The induced E fields are symmetrical in direction about the vertical (laws of reflection - in optics - same thing).

http://farside.ph.utexas.edu/teaching/302l/lectures/img1298.png
This concept is what you're talking about, correct?

So the ground is necessary to ensure that whatever amount of current flows through the antenna has a return path?
 
  • #18
That's the basics of reflection - in terms of 'rays'. But the same idea of symmetry applies when you draw the wave fronts.
Something will take the currents. Using a ground plane defines where they go - and fixes the impedance.
I have a feeling that you are trying to get into this topic at a level that's too deep for your basic knowledge (a common problem). I suggest you do some more reading round (in receive mode) rather than trying to do it by Q and A. Your Qs are not always too relevant, I think.
 
  • #19
sophiecentaur said:
I have a feeling that you are trying to get into this topic at a level that's too deep for your basic knowledge (a common problem). I suggest you do some more reading round (in receive mode) rather than trying to do it by Q and A. Your Qs are not always too relevant, I think.

You're probably right. What do you suggest I read?
 
  • #20
There are loads of Google hits when you search google with monopole antenna theory etc. but I couldn't find anything that I'd say was just what you want. You really need a book on antenna and propagation theory. I have had many books available to me in the past but no more, I'm afraid, so I couldn't be sure if any book I could name would actually have an explanation in detail about how a ground plane works. Kraus has a well known classic book on antennae - written when your granny was a girl, no doubt - but it's a good source for generally reliable stuff about such things. You need something old and dusty, found in the corner of a s/h book shop, perhaps.

It's normally taken as 'a given' that an image is formed but it should suffice to say that a reflection of any frequency of radiation should be expected to form an image in the same way - due to the currents (no details needed) induced in it. If you can believe it works optically (you can see it does) then you should be able to accept it works at MF, too and produces an image in the same way. The image and the monopole go together to form the overall pattern. In the case of a vertical monopole, the virtual currents in the virtual image are the right way to enhance the field in the horizontal direction. However, it may be interesting to note that a horizontal radiator, over a ground plane, produces an image in which the virtual currents (which are in the opposite direction) serve to cancel the radiated field in the horizontal direction. HF antenna arrays deliberately use HP for this reason because they need to fire upwards to the sky and suppress the 'groundwave'.
 
  • #21
Intuitive understanding involves thinking of the ground-plane as a mirror.
The mathematical understanding involves the solution of boundary conditions by the method of images.
The EM understanding involves the electrical currents induced in the ground-plane and the virtual underground image that appears.

http://en.wikipedia.org/wiki/Method_of_image_charges
http://en.wikipedia.org/wiki/Monopole_antenna#Radiation_pattern

The quarter wave monopole radiates as a single element. It is driven relative to the ground plane. The mirror image is “seen” as an inverted element underground. That array of two radiating elements is seen to produce a field identical to a half wavelength dipole.

d.arbitman said:
I don't understand how the reflected portion of the signal constitutes the other 1/4 length of a dipole.
Is that still the problem? Or what do you not understand?
 

Related to Why is a 1/4 wavelength antenna limited to 1/4 wavelength length?

What is a 1/4 wavelength antenna?

A 1/4 wavelength antenna is a type of antenna used in radio communication that is one-quarter the length of the radio wave it is designed to receive or transmit. It is typically made of a conductive material such as metal and is used to convert radio frequency energy into electrical signals, or vice versa.

How does a 1/4 wavelength antenna work?

A 1/4 wavelength antenna works by using the principle of resonance, where the length of the antenna is equal to one-quarter the length of the radio wave it is designed to receive or transmit. This allows the antenna to efficiently send or receive signals at a specific frequency, making it an ideal choice for radio communication.

What are the advantages of using a 1/4 wavelength antenna?

One of the main advantages of a 1/4 wavelength antenna is its compact size. Due to its length being only one-quarter of the radio wave it is designed for, it takes up less space compared to other types of antennas. Additionally, it has a high level of efficiency and can be easily matched to the desired frequency, making it a popular choice among radio communication systems.

What are the applications of a 1/4 wavelength antenna?

1/4 wavelength antennas have a wide range of applications in radio communication, including radio broadcasting, mobile devices, wireless communication, and amateur radio. They are also used in various industries such as aviation, military, and maritime for reliable and efficient communication.

How do I choose the right 1/4 wavelength antenna for my needs?

The right 1/4 wavelength antenna can be chosen based on the frequency range, gain, and impedance required for your specific application. It is important to consider the materials used, construction quality, and compatibility with your radio equipment when selecting a 1/4 wavelength antenna. Consulting with a professional or conducting research can also help in choosing the best antenna for your needs.

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