@gambit
Can you elaborate resonance region?
Actually I am interested in this part
When the target is smaller than the transmitting wavelength, the target's RCS is said to be in the Rayleigh region. The body's RCS is less than its actual physical dimensions.
2- When the body is within about %10 in dimensions of the transmitting signal, it is said to be in the resonance region. Its RCS tends to be larger than its physical dimensions. If the body is irregular, like an aircraft, then the RCS signal would fluctuate.
Point 1 says that when target is smaller than wavelength, its RCS is smaller than physical dimension, but point 2 says that when target is 1/10 of the wavelength, RCS is larger than physical dimension.
Both points seem contradictory, unless there is irregularity near the 1/10 region.
Not contradictory at all and this is where you misunderstood me about that 'target is 1/10 of the wavelength' bit. I am saying that target 'electrical path' and the impinging wavelength is roughly within %10 of each other, not that the target, be it a sphere or a raindrop or an insect, is one-tenth in size compared to the wavelength.
First...Keep in mind that radar detection is essentially about perception based upon target characteristics. The advantage that radar detection have over other methods of target detection is that the user control the medium from which the target must respond, in other words, every target reflects some amount of energy. For infrared detection, the user or seeker, does not transmit an 'IR wave' at the target and read the return. The seeker must rely upon the convenience of the target to emit some IR energy.
Second...The perception formulation is no different than how you would formulate a perception of a new acquaintance, like in a date, for example. The formulation is based upon what you received in that meeting, from how was the handshake to the smile or other signs in body language. For radar detection, the formulation is mathematically quantifiable.
Third...The three regions: Rayleigh, resonance and optical, are like those body language signs and they come from how a wave behave on a sphere, an 'ideal' object, which is used as a reference in RCS modeling.
Fourth...There is a 'shadow' region in a monostatic configuration. A monostatic system is the most commonly deployed in the world.
radar shadow: Definition from Answers.com
A region shielded from radar illumination by an intervening reflecting or absorbing medium such as a hill.
You will have to excuse my pathetic 'artistic' skills here.
The side that is not illuminated by the seeker is the 'shadow' region as illustrated above.
Fifth...Any reflection that is facing the seeker, up until the 90deg point, is called a 'backscatter' as illustrated above. Any reflection beyond that 90deg point is called a 'forwardscatter'. In a monostatic configuration, only 'backscatter' reflections are useful in RCS calculations.
Upon impacting the surface of the sphere, there is an immediate amount of reflectivity back to transmit direction. This initial reflection is called 'specular' reflection. The rest of the signal then travels on the sphere's surface. At this point the sphere's diameter comes into play regarding wavelength. The sphere's diameter is called the 'electrical path' and does have a length. As the signal travels on the surface in the 'creeping wave' effect, minute amount of the signal's energy reflects off the surface, aka more 'specular' reflections.
If the sphere's diameter is smaller than the impinging wavelength, after the initial 'specular' reflection, there is a 'creeping wave' behavior and most of the signal will complete its travel on the sphere's surface, reform on the shadow region and become a 'forward scatter'. All the seeker radar has are the few 'backscatter specular' reflections to formulate a perception of the target's physical dimension. This is why target RCS in this ratio is less than what the target actually look like -- size wise. The target is said to be in the 'Rayleigh' region. If we have meters wavelength hitting a raindrop or an insect neither would show up at all.
If the sphere's diameter is the same as the impinging wavelength, once the wave finally completed its travels around the sphere and the 'creeping wave' meets on the back side, aka the 'shadow' region, we have lost not as much of the signal to 'forwardscatter' as when the sphere was smaller than the wavelength. The 'resonance' effect is the result of in-phase and out-of-phase interference between the many 'specular' reflections and the 'creeping wave' behavior, hence, target RCS from this 'electrical path' versus wavelength relationship varies a great deal and generally indicate a target RCS that is larger than its physical dimension. This in-phase and out-of-phase interference has two results: constructive and destructive, and it does exist in the above Rayleigh region example as well, except that because the above example has the sphere's diameter smaller than the impinging wavelength, the 'creeping wave' interference is usually destructive. As sphere diameter increases, then we approaches the resonance region.
If the sphere is large enough, in other words the 'electrical path' is greater than wavelength, then eventually the entire signal never complete its travel around the sphere before all of its energy is spent thru these many 'specular' reflections. So if the sphere is larger than wavelength, its RCS will appear, or more precisely 'perceived', to be cumulative of these 'specular' reflections and is more approximate, never precise, of the sphere's physical diameter. Remember, the ideal situation is to have %100 of the signal's energy back to the seeker, so we want to gather as much of the signal's many 'specular' reflections as possible before any part of the 'creeping wave' travels to the 'shadow' region.
The sphere is used precisely because it is an ideal object and with other simple objects like the cylinder or a plane we can create references upon which to 'decompose' complex bodies and perform minor RCS calculations upon them. The trick later is on how to recomposite all these discrete simple RCS results into a larger complex one and hopefully it will yield us an accurate overall RCS.
Also, can you give details on this?
Rayleigh scattering? This should be in your physics class.
Rayleigh wave - Wikipedia, the free encyclopedia
I have worked on increasing absorption by decreasing of target size (though in different region).
I am interested to know if absorption can be decreased.
Not exactly certain what you are talking about here.