EM re-radiation from a metal object (antennas)

In summary, two identical monopole antennas placed in a field with distance d are used to receive signals. One of them is disconnected and considered to be just a metal rod. A plane wave of a single frequency from a distant source is received and the disconnected antenna is expected to re-radiate most of the energy it receives. The contribution of the re-emitted wave will depend on the inverse square law and the aperture of the receiving antenna. It is possible to minimize the re-radiation by detuning the antenna with an inductive-capacitive network. The passive antenna can develop the same EMF as the active one and the current is determined by its radiation resistance and load resistance. If the passive antenna is disconnected, it will
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Johan L
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Consider the following situation. Two identical monopole antennas are placed in a field with distance d. One of them is used to receive signals and the other is disconnected and can therefor be considered to be just a metal rod (my guess). A plane wave of a single frequency is coming from a distant source. Since no energy is extracted in the form of a signal from the passive antenna I guess it will re-radiate most of the energy received by it (minus thermal dissipation). Questions:

Is it first of all true that a disconnected antenna re-emits most of the energy that otherwise would have been absorbed and converted into a signal?

How strong will the contribution of the re-emitted wave be compared to the original for the receiving antenna? Is it just a a matter of the inverse square law and the aperture of the receiving antenna?

Can you prevent the passive antenna from re-emitting totally (and over all frequencies) by terminating it somehow?
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I think the best you can hope for is to minimize the current in the metal pole by de-tuning it with an inductive-capacitive network. This reradiation issue is a problem with cell towers located near am broadcast stations and there are companies that manufacture "detuning skirts" to minimize reradiation form the am broadcast station.
 
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The passive antenna develops the same EMF at its terminals as the active one, so the current is determined by its radiation resistance and load resistance in series. If the passive antenna is disconnected it has no current, so it will not influence the received power of the active one. If it is short circuited it will carry a large current and will re-radiate all the "incident" power. The phase of the radiation depends on the ratio of reactance to resistance for the passive antenna; this is the basis of the Yagi antenna, where an inductive antenna acts as a reflector and a capacitive antenna acts as a director.

To ascertain the effect on the active antenna, the usual way is to look up curves for the mutual impedance and apply a formula for coupled cciruits. Altenatively, the path loss formula can be used if the spacing is greater than about lambda/6. If it is closer than this, the attenuation between the two will be nominally 3dB. It is necessary to take into account the phase of the two signals during addition.
 
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Yagi TV antennas have numerous horizontal dipoles. usually only one of these is connected to the receiver. The others are called parasitic elements. These extra passive elements increase the active dipoles directivity by 20 to 30 dB.
 
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I think the 20 to 30 dB figure is a little high. More usually abouit 15 dB. To obtain 30dB directivity increase would require about 1000 dipoles.
 
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tech99 said:
If the passive antenna is disconnected it has no current, so it will not influence the received power of the active one. If it is short circuited it will carry a large current and will re-radiate all the "incident" power.
Thanks for the explanation. But this makes me a bit confused. Doesn't an electromagnetic wave always induce current to flow back and forth in a thin solid linear conductor (assuming it is directed along the E-field)? With a resonance maximum when the conductor is λ/2 long?

Can't a solid linear conductor of length L that is disconnected from the ground be considered to be a "short circuited" dipole with two conductors of length L/2? So if a wave impinges on a thin metal rod, in my mind it will then (according to the second sentence in the quote above) re-radiate all incident power if the wavelength is twice that of the rod. Or am I missing something?
 
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Johan L said:
Thanks for the explanation. But this makes me a bit confused. Doesn't an electromagnetic wave always induce current to flow back and forth in a thin solid linear conductor (assuming it is directed along the E-field)? With a resonance maximum when the conductor is λ/2 long?

Can't a solid linear conductor of length L that is disconnected from the ground be considered to be a "short circuited" dipole with two conductors of length L/2? So if a wave impinges on a thin metal rod, in my mind it will then (according to the second sentence in the quote above) re-radiate all incident power if the wavelength is twice that of the rod. Or am I missing something?
Your heading mentions monopoles, so my explanation refers to monopoles which I assume to be a quarter of wavelength long. Such an antenna utilises the ground as one terminal. If the monopole is half a wavelength long then it can be resonate without the ground plane, so to disable it would require breaking it at the mid point.
 
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Johan L said:
Can't a solid linear conductor of length L that is disconnected from the ground be considered to be a "short circuited" dipole with two conductors of length L/2?
That's a very interesting way of seeing it but in my opinion it is not the same thing as a short circuited dipole. In my opinion the two ends of the conductor form a capacitor (that has as in between space all the surrounding space) that has some small capacitance so the circuit is "closed" via this small capacitor and the current in the circuit (which consists of the rod plus this capacitor) is minimized because of this small capacitance.
 
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tech99 said:
Your heading mentions monopoles, so my explanation refers to monopoles which I assume to be a quarter of wavelength long. Such an antenna utilises the ground as one terminal. If the monopole is half a wavelength long then it can be resonate without the ground plane, so to disable it would require breaking it at the mid point.
Ok. should have been clearer about that. Then we agree.

Delta2 said:
That's a very interesting way of seeing it but in my opinion it is not the same thing as a short circuited dipole. ...
Not sure I follow your analogy with a capacitor. Are you thinking of the circuit equivalent of a dipole antenna? Do you not consider the two arrangements below to be "equivalent"? That the same current will flow inside the antenna element(s), even when the frequency is not perfectly tuned? If one re-emits all the energy that it absorbs, will not the other (minus thermal losses)?

How much that is absorbed on the other hand (how much current that is generated), should depend on the frequency right? The antennas should be "invisible", and the surrounding EM plane wave field should not be much effected by them, for frequencies far away from the resonance, no?

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Johan L said:
Do you not consider the two arrangements below to be "equivalent"?

If you consider the left antenna or the right antenna in the figure below independently for reflection and scattering of electromagnetic wave from space, and they have the same size and shape (including length, diameter, and the gap between the lower end and the ground, etc.), then I can't see any reason why they are not equivalent.

But If the distance between the lower end of the right antenna and the ground is much greater than that of the left antenna, or if you consider that the feeding point of the left antenna is at the bottom and the feeding point of the right antenna is in the middle, etc., then of course they cannot be equivalent.

So whether the two are equivalent depends on the specific situation and how we consider it. :smile:
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The two are not the same. The RH version is isolated from ground, so its lowest resonance is when it is half a wavelength long. The LH version is connected to ground, so its lowest resonance is when it is a quarter wavelength long ie half the frequency. When the switch is open they are the same.
 
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tech99 said:
The two are not the same. The RH version is isolated from ground, so its lowest resonance is when it is half a wavelength long. The LH version is connected to ground, so its lowest resonance is when it is a quarter wavelength long ie half the frequency. When the switch is open they are the same.
What you say is correct. However, it doesn't just apply at Resonance, although the currents at resonance can be much higher. Any piece of metal will have currents induced in it by an incident EM wave and, even if the 'parasitic' dipole is open circuit at the middle (therefore well away from resonance), it will / can affect the net induced emf in a nearby receiving antenna. If you really need to eliminate such effects (such as in the stays of a tall MF mast antenna) the parasitic structure would be divided up into much shorter lengths with insulators. (Something to spot when driving past some MF local radio masts)

Many dipole antennae are mounted, stood - off from a mast part way up and the (sometimes very wide) mast is a significant element in the antenna pattern. In that case, the 'reflector' is very long and well away from resonance. Choosing the right spacing can give some useful control of the horizontal pattern.
 
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tech99 said:
The two are not the same. The RH version is isolated from ground, so its lowest resonance is when it is half a wavelength long. The LH version is connected to ground, so its lowest resonance is when it is a quarter wavelength long ie half the frequency. When the switch is open they are the same.
I made the switch open so that it would depict the situation when they are the same.
 
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Johan L said:
I made the switch open so that it would depict the situation when they are the same.
The presence of the ground (explicit on the left) effectively places an Image of the antenna underground because of the part of the wave front that hits the ground and reflects upwards (at an angle) towards the antenna itself (one way of thinking of it). It gives a Vertical Pattern that's different from that of an isolated antenna, out in empty space (or a few wavelengths up).
 

FAQ: EM re-radiation from a metal object (antennas)

What is EM re-radiation from a metal object?

EM re-radiation from a metal object refers to the phenomenon where an electromagnetic (EM) wave is emitted from a metal object, such as an antenna, due to the interaction between the EM wave and the metal. This can occur when the metal object is exposed to an external EM field or when an electrical current is passed through it.

How does EM re-radiation affect the performance of an antenna?

EM re-radiation can have both positive and negative effects on the performance of an antenna. On one hand, it can increase the efficiency and gain of the antenna by redirecting the EM energy in a desired direction. On the other hand, it can also cause interference and reduce the signal strength if not properly controlled.

What factors can influence the amount of EM re-radiation from a metal object?

The amount of EM re-radiation from a metal object can be influenced by several factors, including the size and shape of the object, the material it is made of, the frequency of the EM wave, and the surrounding environment. These factors can affect the resonant frequency, impedance, and radiation pattern of the antenna, ultimately affecting the amount of EM re-radiation.

How can EM re-radiation be controlled in an antenna?

EM re-radiation can be controlled in an antenna through various methods, such as using proper shielding and grounding techniques, designing the antenna with specific dimensions and materials, and using filters and baluns to reduce unwanted radiation. Additionally, the placement and orientation of the antenna can also play a role in controlling EM re-radiation.

Is EM re-radiation from a metal object harmful to humans?

The amount of EM re-radiation from a metal object is typically very low and is not considered harmful to humans. However, it is always important to follow safety guidelines and regulations when working with antennas and other electronic devices to minimize any potential health risks.

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