Skin RCS reduction :
No matter what shape they have, airframe will always reflect radar waves.The only different that shaping will make is the directions that the airframe will reflect radar.Whilethis may be enough in most situation.The adversary may consist of very complex radar network that can illuminate stealth platform from different angles, so along with unique shaping to redirect radar wave from the original source, stealth aircraft often have radar absorbing paint or use radar absorbing material (RAM ).One might be very tempted to construct stealth aircraft skin from such “radio transparent” materials, but radar would then reflect off objects beneath the surface such as sensors, fuel, metallic airframe and engine parts and the pilot.The result may be a RCS value even higher than if the skin was radar reflective. As a result, in practice, the bottom layer of a stealth skin is a highly conductive material, such as metal, which strongly reflects radar waves before they reach the complex reflecting environment below.
The ability of a substance to absorb electromagnetic (EM) waves depends on two material properties called permittivity and permeability, which are the capacity to store electrical or magnetic energy, respectively. The source of both is the existence of electric or magnetic dipoles at the atomic, molecular or crystal lattice level. When an EM wave passes through the material, these dipoles orient opposite to the field’s direction. In some materials, the dipoles effortlessly return to neutral after the EM field returns to zero. In other materials, the dipoles are “sticky” and require energy to orient them or return them to neutral. That additional energy is lost and the material’s permittivity or permeability is said to have a loss component.
In general, RAMs are composites made up of a matrix material and a filler. The matrix is a low-loss dielectric material with appreciable permittivity and negligible permeability. They are effectively “transparent” to EM waves and are usually chosen for their physical properties. Typically, they are insulating polymers like plastic, glass, resin, polyurethane and rubber. Ceramics have higher permeabilities and heat tolerance. Foams and honeycombs have especially low permittivity—electrical energy storage—because they contain a lot of air.The RAM filler, on the other hand, is typically particles composed of or coated with a lossy material. Carbon is the material of choice for dielectric absorption because electrical lossiness is proportional to conductivity and carbon’s conductivity is below metals but above insulators. Magnetic absorbers, which have some permittivity but far greater permeability—magnetic energy storage—are typically carbonyl iron (a pure powdered form of the metal) or iron oxides, also called ferrites. These materials can be impregnated into rubber or dissolved into a paint and ferrites are often sintered into tiles.
As its permittivity, permeability, and loss components increase, a material can absorb more EM energy because EM wavelengths shrink as these values rise. But when waves reach a boundary between two mediums, energy can be reflected rather than admitted. The amount reflected depends on their impedances—the square root of the ratio between each material’s permeability and permittivity. The greater the impedance change, the more energy is reflected before it can be absorbed. So RAM design must balance absorptivity with surface reflectivity to maximize absorption.
A material’s EM properties also varied significantly with frequency. At higher radar bands, no magnetic materials have permittivity and permeability in a ratio close to that of air, so high surface reflection is inevitable. However, if the material is a quarter-wavelength deep, reflection from the metal backing partially cancels the surface reflection.Radarabsorbing materials operate via phase cancellation like this is often called magnetic absorber. Because of the high permeability of magnetic RAM, the depth required is small. Absorption performance of 20 dB (99%) is achieved by commercially available “resonant absorbers” with resonant frequencies of 1-18 GHz and thicknesses of 0.04-0.2 in. The main disadvantages of such absorber is very narrow absorbing bandwidth, however, with significant absorption extending perhaps 15% from the resonance frequency.
Given that magnetic absorbing material has limited bandwidth, as well as high weight and cost, dielectric absorbers are often preferred for wideband absorption at high frequencies. Since dielectrics have no magnetic properties, their impedances never match air, but by using layers of materials—each with an increasing concentration of carbon particles—permittivity, conductivity and dielectric losses all gradually increase while impedance gradually decreases. Layers can also be adjusted to maximize cancellations. These graded dielectric absorbers can reduce reflection by 20 dB, and their bandwidth easily covers higher frequencies. High levels of reflection loss, in many cases better than 20dB, can be achieved in materials which are <1/3 wavelength thick. One of the most common type of graded dielectric absorber is the reticulated foam absorbing material.
Another approach is to use a physical gradient. These “geometric transition” absorbers use pointed objects of homogeneous material oriented perpendicular to waves. At high frequencies, waves bounce among these structures, losing energy with each strike. If the wavelength is large relative to the structure, the waves act as though encountering a gradual change in material properties rather than a geometric shape. Absorbers of this type can reduce reflection by up to 60 dB, but require structures very big structures and high weight so their only application is the pyramidal absorbers that line anechoic chambers used for RCS testing.
It is a common misconception that radar absorbing material is only effective around X band (8-12 Ghz) or that RAM work at low frequencies will always need to be thick or heavy. In fact, some magnetic materials actually become more effective at lower frequencies because their energy storage (permeability) increases. At frequencies of 30-1,000 MHz, certain ferrites exhibit extreme wave compression and impedance close to air. Commercial ferrite tiles can achieve over 20 dB reduction in VHF band and 10 dB reduction through UHF, with a thickness of only 0.25 in. and a weight of 7 lb./ft.2.
So far, what has been discussed is reducing specular reflections—those that bounce off an object like light off a mirror—but RAM is also particularly effective at reducing surface waves. These are the waves emitted by currents induced in a conductive surface when struck by radar. As they move along the surface they emit traveling waves, usually at angles close to grazing, and when they encounter discontinuities—an airframe edge, a gap or step in the surface or a change in material—they emit edge waves, concentrated closer to the specular reflection. Surface currents travel along a material’s length rather than through its thickness, and the RAM acts as a waveguide, trapping the currents and absorbing them. Magnetic RAM can suppress surface currents well in a thickness of only 0.03 in. There are ways to combine techniques. Layered magnetic materials can reduce RCS by 10 dB from 2-20 GHz with 0.3 in. of depth. Hybrid RAMs can be created with a front layer of graded dielectric and a back layer of magnetic material to attenuate radar reflections from VHF to Ku-band (30 MHz-18 Ghz).
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