Electromagnetic Stealth -The Fight Against Radar

Electromagnetic Stealth -The Fight Against Radar

Electromagnetic Stealth : The Fight Against Radar 2011142159 Jang Yune-seok 2012142168 Lee Jun-hyuk [Introduction] [Introduction] · How Radars locate targets? : in angle and distance. [Introduction] · How to avoid detection : Minimizing visual signature, infrared heat signature, acoustic signature, radio transmission signature and radar echo signature using a variety of advanced technologies. · The goal of stealth technology : Invisible to radar using principle of reflection. ⅰ) Shaped so that any radar signals are reflected away from the radar equipment. ⅱ) Covered in electromagnetic absorbing materials. [Radar Cross Section] [Radar Cross Section] · RCS(Radar Cross Section) : Measure of how detectable an object. A large RCS indicates that an object is more easily detected. - The RCS depends on - Shape of the target - Absolute size of the target - Material of the target - The incident and reflected angle [Radar Cross Section] · How to calculate RCS 2 RCS σ = 4·π·r s /s r t st : power density that is intercepted by target sr : scattered power density in the range RCS of Various Flying Objects Object RCS[m²] F-15 Eagle 405 B-1A 10 SR-71 Blackbird 0.014 Birds 0.01 F-117 0.003 B-2 Sprit 0.0014 Insects 0.001 [Radar Cross Section] · How to calculate RCS 2 RCS σ = 4·π·r s /s r t st : power density that is intercepted by target sr : scattered power density in the range RCS of Various Flying Objects Object RCS[m²] F-15 Eagle 405 B-1A 10 SR-71 Blackbird 0.014 Birds 0.01 F-117 0.003 B-2 Sprit 0.0014 Insects 0.001 [Design of stealth] Shape And Material Shape And Material [Shape] The past The present The future [Shape] Diamond shape The curved shape The diamond shape [Shape] Diamond shape The curved shape The diamond shape [Shape] · Engine inlet design : Buried engine [Shape] - Disadvantage of diamond shape 1. Poor aerodynamics. 2. Poorly reducing RCS of bistatic radar system. Shape And Material [Material] · Non-conductive material Reflection coeffcient Reflected power n2p – n1p Pr Γp = = |Γp|² n2p + n1p Pinc n2s – n1s Pt Γs = = 1 - |Γp|² n2s + n1s Pinc n1 = n2 ⇒ Γp = 0, Γs = 0 [Material] · Radar Absorbing Material (RAM) : Absorption the energy of the radio waves transmitted by the radar antenna. [Carbonyl iron ferrite] [Material] - Frequency selective surface(FSS) : FSS is designed to improve the wideband stealth performance of RAM. [The structure sketch map of RAM containing FSS] [The equivalent circuit model] Reflection coefficient of RAM : [Material] - Frequency selective surface(FSS) We optimize the FSS element design based on the electromagnetic parameter of RAM. [Material] - Multi-layer RAM The reflection is calculated as The reflection coefficient of RAM is a multi-variable function. The optimal variables of the parameters only be obtained by optimized algorithms. [Plasma stealth] [Plasma stealth] [Plasma stealth] · Why stealth make plasma? 1. The absorption take place when EM wave encounter a charged particle. 2. Electromagnetic wave tend to bend around the cloud and pass aircraft. 3. Frequency oscillation of a plasma changes frequency of incoming radar waves which makes radar waves to become useless. Advantages Disadvantages 1. Radar Absorption Material is not 1. Making plasma cloud around needed. aircraft require huge power. 2. Plasma will provide heat shield 2. Plasma layer can also block pilot’s which separate plane from hot air. radar. 3. Plasma could soften airflow across 3. When ion is neutralized it will give the aircraft so aircraft could be off light It will create visual path of more aerodynamic. aircraft [Plasma stealth] - Absorption of Electromagnetic wave by plasma [Plasma stealth] In collisional plasma electron under EM-wave can express by If we consider E as exponential form, collision frequency is By maxwell equation we can get wave equation as We can get dispersion equation by J=nev If plasma is collisional ν is not zero and ki is positive, E-field is absorbed by plasma. [Plasma stealth] - Refraction of Electromagnetic wave by plasma [Plasma stealth] When plasma collision is omitted, it’s refraction index is If plasma density changes with R, We combine two equation. We can get EV-wave’s R and θ. We can get C1, C2 by substitute R0 and EM-wave’s incident angle. Based on Snell’s law, we can get [Conclusion] [Conclusion] [Radar] vs [Stealth] Thank you! .

View Full Text

Details

  • File Type
    pdf
  • Upload Time
    -
  • Content Languages
    English
  • Upload User
    Anonymous/Not logged-in
  • File Pages
    32 Page
  • File Size
    -

Download

Channel Download Status
Express Download Enable

Copyright

We respect the copyrights and intellectual property rights of all users. All uploaded documents are either original works of the uploader or authorized works of the rightful owners.

  • Not to be reproduced or distributed without explicit permission.
  • Not used for commercial purposes outside of approved use cases.
  • Not used to infringe on the rights of the original creators.
  • If you believe any content infringes your copyright, please contact us immediately.

Support

For help with questions, suggestions, or problems, please contact us