Difference between revisions of "Application Article: Modeling Large Structures in EM.Tempo"

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== Introduction ==
 
== Introduction ==
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In this article, we compute the bistatic radar cross-section (RCS) of a Dassault Mirage III type fighter aircraft at 850 MHz.  At 850 MHz, the aircraft is about 42 freespace wavelengths long,
  
  

Revision as of 19:42, 7 October 2016

Application Project: Radar Cross-Section of Aircraft
Large struct article ScreenCapture3.png

Objective: In this article, we explore computing RCS of electrically large structures, like aircraft.

Concepts/Features:

  • Radar Cross Section
  • Large Projects
  • Cloud-Based Resources

Minimum Version Required: All versions

'Download2x.png Download Link: None

Introduction

In this article, we compute the bistatic radar cross-section (RCS) of a Dassault Mirage III type fighter aircraft at 850 MHz. At 850 MHz, the aircraft is about 42 freespace wavelengths long,


Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.


Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.


Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.


Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.


Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.
Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.
Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.
Figure 1: Geometry of the periodic unit cell of the dispersive water slab in EM.Tempo.