How EMR interacts with matter and how antennas differ to other rods

In summary: I'm saying that the antenna will resonate with a frequency that is related to the physical dimensions of the antenna itself, but what about all the other frequencies, are they attributable to the connected tuning circuit?No, the other frequencies are not related to the connected tuning circuit.
  • #1
toneboy1
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Hi,
So I was thinking, if you've got a metal rod of random size, then any EMR wavelength that the rod (antenna) is a similar length to will stimulate an AC current inside the rod as a complete mess. (It would be the sum of all the frequencies the rod can resonate with)
IS THIS ACCURATE??

But THEN you put an LC circuit on the end of the rod and you tune it (the LC circuit becoming in essence part of the rod! (antenna)) so that ONLY ONE frequency now resonates in the rod.
IS THIS ACCURATE??

If so, how would a one atom antenna resonate? A frequency the wavelength of the atom?
Is the difference between an antenna and other matter that it resonates from EMR but a person doesn't?
 
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  • #2
EDIT - corrected
 
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  • #3
So a rod is a complete non-resonating mess? But an antenna obviously, resonates.
 
  • #4
toneboy1 said:
So I was thinking, if you've got a metal rod of random size, then any EMR wavelength that the rod (antenna) is a similar length to will stimulate an AC current inside the rod as a complete mess. (It would be the sum of all the frequencies the rod can resonate with) IS THIS ACCURATE??

But THEN you put an LC circuit on the end of the rod and you tune it (the LC circuit becoming in essence part of the rod! (antenna)) so that ONLY ONE frequency now resonates in the rod.
IS THIS ACCURATE??
In the absence of another nearby conducting object, the only currents I think will be induced in your rod are Eddy currents. If, on the other hand, you rod is connected to a receiver then the rod is a monopole antenna where the AC current will be capacitively coupled to the the reference plane (e.g., ground) to complete the circuit. The rod has resistance and inductance which means you'll have a series RLC circuit which in turn has a resonant frequency that is equal to a quarter wavelength.
 
  • #5
FOIWATER said:
antenna act the way they do because of the skin effect. [...] The antenna picks up all frequencies of radio, not just one, the wavelength need not be "similar" to the length of the antenna...
I think it's a stretch to say that antennas act as they do because of the skin effect. I'm also not sure what your trying to point out re the length of an antenna---the amount of energy you can put into or take out of an antenna is obviously related to the self-resonance, and hence electrical length, of the antenna. Maybe we're not on the same page here? :)
 
  • #6
I'm not sure what the "skin effect" has to do with the way you can analyse the behaviour of a transmitting or receiving antenna.

Any piece of metal will interact with any em wave that happens to be passing by. It will modify the fields appreciably if it happens to resonate (in some way) at the frequency of the wave and this can reflect or deflect the wave. If you put an appropriate resistor (load) across certain parts of the piece then energy will be dissipated in the resistor. The piece of metal need not actually be self-resonant if you add the appropriate values of lumped reactive components into the circuit. Getting significant power into or out of an antenna of the 'wrong size and shape' may involve a great deal of power loss. Short monopoles tend to be inefficient but you can't make a quarter wave radiator at 200kHz so you just have to put up with it.
Essentially, you can match any frequency into the proverbial 'dead sheep' and get it to act like some sort of an antenna - but not a good one.
 
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  • #8
Ok, I see what the OP means, once the circuit is tuned, it in essence becomes part of the antenna, and resonance only then occurs at one frequency,

I never thought of it that way before, but I see what you mean.
 
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  • #9
FOIWATER said:
Ok, I see what the OP means, once the circuit is tuned, it in essence becomes part of the antenna, and resonance only then occurs at one frequency.
The antenna is also self-resonant at a frequency that is related to the physical dimensions of the antenna itself.

Also, by going back and deleting your posts you're removing the context from other commenter's posts and making the thread incomprehensible.
 
  • #10
ok

so it is resonant with that frequency, the one attributable to the physical dimensions of the antenna itself, but what about all the other frequencies, are they attributable to the connected tuning circuit?

The OP asked if all frequencies would induce voltage into the antenna as a kind of "mess"

Are you saying that is not true, that there is one resonant frequency, and many other possible "tuned" frequencies?

I'm not sure..
 
  • #11
You seem to be drawing too much of a distinction between the piece of metal and other 'pieces' of metal (such as coils and capacitors) that happen to be connected to it. In many cases, there is not such a clear distinction. Look at a base loaded monopole, for instance, that has a coil at its base which may constitute up to 10% of its height - or a top (capacity) loaded , 'T' antenna. Sometimes (often, even) it is possible to treat the antenna and its matching circuit as two separate elements but it isn't fundamental.
What counts is the currents that happen to be flowing in large parts of the structure and the way it's built will affect them.
Usually, the last thing you want is for your antenna to be highly tuned. Wide band is usually what you are after and wide band matching is a serious engineering art.
 
  • #12
sophiecentaur said:
...
What counts is the currents that happen to be flowing in large parts of the structure and the way it's built will affect them.
Usually, the last thing you want is for your antenna to be highly tuned. Wide band is usually what you are after and wide band matching is a serious engineering art.

Well say we were comparing three things: a single atom (with I suppose no inductive or capacitive capability), an antenna we wanted to suit only one frequency and another we wanted to match a wide band of frequencies.
So the inductive / capacitive capabilities of: the first would mean the electrons didn't resonate with any EMR, the second did best for only frequencies related to the fraction of antenna length to wavelength and the third could selectively resonate the electrons depending on how the LC of the antenna (and circuit) were tuned?

Is that an accurate statement?

Thanks!
 
  • #13
I think you are trying to reconcile two different models when what you are really dealing with is the old Duality thing. You either must talk about photons or about waves - choose.
The electrons can be regarded as resonating in a simple atom structure because you have line spectra and discrete energy levels; it is ok to discuss photon - atom interaction in that case. You do not have discrete energy levels in condensed matter (Pauli exclusion principle applies to Fermions so you end up with broad bands and not levels) and you need to talk in terms of the photons interacting with the whole structure (distributed charges throughout the antenna) and not individual electrons, in which case, any resonance will the the same as that which classical wave theory will give you (you can't solve it with quantum mechanics afaik).
 
  • #14
sophiecentaur said:
I think you are trying to reconcile two different models when what you are really dealing with is the old Duality thing. You either must talk about photons or about waves - choose.
The electrons can be regarded as resonating in a simple atom structure because you have line spectra and discrete energy levels; it is ok to discuss photon - atom interaction in that case. You do not have discrete energy levels in condensed matter (Pauli exclusion principle applies to Fermions so you end up with broad bands and not levels) and you need to talk in terms of the photons interacting with the whole structure (distributed charges throughout the antenna) and not individual electrons, in which case, any resonance will the the same as that which classical wave theory will give you (you can't solve it with quantum mechanics afaik).

1. What exactly do you mean by 'broad bands'? Like voltage nodes along the antenna?
2. I was looking up the Pauli exclusion principle, but I don't see how not occupying the same state means they are 'broad bands' (?)
3. To get a general idea. What sort of distance are these charges oscillating back and fourth on the antenna? Any analogy to relate it you like.

Thanks heaps for helping me get my head around this!

EDIT - How should I visualize the charges moving on the antenna as a wave?
 
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  • #15
Broad bands: Nothing to do with antennae - it's to do with energy (Quantum) levels. You've heard of the discrete energy levels in the simple Hydrogen atom? Condensed materials don't have single energy levels, they have a continuous range of possible energies - referred to as bands. Pauli applies because they can't all occupy the same state and a single line (corresponding to one state) will be broadened to allow all the closely spaced atoms to get somewhere near the level they would be in if they were on their own.

This isn't going to help at all if I tell you that the charges have virtually no movement at all. If you consider that the drift speed of electrons is a couple of mm/s and then you realize that, at 10MHz, they are changing direction every 10 millionth of a second. The ain't going to get far in that time and at that speed!
The secret of getting this stuff is to use the right terms and not your own ones. When you talk of antennae, you need to drop QM and use Currents, Potential Differences, Electric Fields and Magnetic Fields. There is an almost simultaneous thread in which we are trying to put to bed the idea that moving charges and their speeds are at all relevant. See: this.
 
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  • #16
sophiecentaur said:
Condensed materials don't have single energy levels, they have a continuous range of possible energies - referred to as bands. Pauli applies because they can't all occupy the same state and a single line (corresponding to one state) will be broadened to allow all the closely spaced atoms to get somewhere near the level they would be in if they were on their own.
... There is an almost simultaneous thread in which we are trying to put to bed the idea that moving charges and their speeds are at all relevant. See: this.

That makes a lot of sense being tightly packed! Cool
Oh, yes that thread, I am familiar with that, I'll continue on there. Cheers
 

FAQ: How EMR interacts with matter and how antennas differ to other rods

1. How does electromagnetic radiation (EMR) interact with matter?

EMR interacts with matter through a process called absorption, where the energy from the radiation is transferred to the atoms or molecules of the matter. This can cause the particles to vibrate, creating heat, or it can excite electrons, causing them to move and potentially creating an electrical current.

2. What determines the interaction of EMR with matter?

The interaction of EMR with matter depends on the frequency and wavelength of the radiation. Different types of EMR, such as radio waves, microwaves, infrared, visible light, ultraviolet, X-rays, and gamma rays, have different wavelengths and frequencies, and therefore interact with matter in different ways.

3. How do antennas differ from other rods?

Antennas and other rods differ primarily in their shape and function. Antennas are specifically designed to transmit or receive electromagnetic waves, while other rods may have different purposes, such as supporting structures or conducting electricity. Additionally, antennas are generally longer and thinner than other rods to optimize their interaction with EMR.

4. How do antennas work?

Antennas work by converting electrical signals into electromagnetic waves or vice versa. They typically consist of a conductive material, such as metal, that is connected to an electrical circuit. When an alternating current flows through the circuit, it creates an electromagnetic field around the antenna, which then radiates the energy as EMR.

5. What are the applications of EMR and antennas?

EMR and antennas have a wide range of applications, including communication systems (such as radio, TV, and cell phones), medical imaging (such as X-rays and MRI), and scientific research (such as studying the properties of matter and detecting distant objects in space). They also play a crucial role in everyday devices such as microwaves, remote controls, and Wi-Fi routers.

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