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EEE381B Aerospace Systems

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Title: EEE381B Aerospace Systems


1
EEE381BAerospace Systems Avionics
  • Radar
  • Part 2 The radar range equation
  • Ref Moir Seabridge 2006, Chapter 3,4

2
Outline
  • Basic radar range equation
  • Developing the radar range equation
  • Design impacts
  • Receiver sensitivity
  • Radar cross-section
  • Low observability
  • Exercises

3
1. Basic radar range equation
  • There are many different versions of the radar
    range equation.
  • We will use, and fully derive, the one presented
    below.

4
1.1 Components of the equation
  • Rmax the maximum range of the radar
  • Pt average power of the transmitter
  • G gain of the transmit/receive antenna
  • ? wavelength of the operating frequency
  • ? radar cross-section of the target
  • Smin minimum detectable signal power

5
1.2 Units of the equation
6
2. Developing radar range equation
7
2.1 Transmitted power
  • Recall from the previous lecture that the average
    transmitted power is a function of peak pulse
    power and the pulse duration

8
2.2 Power density at target 4
  • Recall that power density decreases as a function
    of distance traveled

9
2.3 Reflected power
  • The amount of power reflected back from a target
    is a function of the power density at the target
    and the targets radar cross-section, ?

10
2.4 Power density of echo at antenna
  • The power density of the returned signal, echo,
    again spreads as it travels back towards the
    radar receive antenna.

11
2.5 Power of echo at receiver
  • The antenna captures only a portion of the echoed
    power density as a function of the receive
    antennas effective aperture

In this equation the receiver is assumed to be
all radar receive chain components except the
antenna.
12
2.5.1 Relative power received ? range
13
2.6 Minimum detectable signal power
  • Therefore a radar system is capable of detecting
    targets as long as the received echo power is
    greater than or equal to the minimum detectable
    signal power of the receive chain

14
3. Radar design impacts
  • A careful study of the radar range equation
    provides further insight as to the effect of
    several radar design decisions.
  • In general the equation tells us that for a
    radar to have a long range, the transmitter must
    be high power, the antenna must be large and have
    high gain, and the receiver must be very
    sensitive.

15
3.1 Power, Pt
  • Increases in transmitter power yield a
    surprisingly small increase in radar range, since
    range increases by the inverse fourth power.
  • For example, a doubling of transmitter peak power
    results increases radar range by only 19,

16
3.2 Time-on-target, ?/Tp
  • The average power transmitted can also be
    increased by increasing the pulse duty cycle,
    sometimes referred to as the time-on-target.
  • A combined doubling of the pulse width and
    doubling of the transmitter peak power will give
    a fourfold increase in average transmitted power,
    and 41 increase in radar range.

17
3.3 Gain, G
  • Antenna gain is a major consideration in the
    design of the radar system.
  • For a parabolic dish, doubling the antenna size
    (diameter) will yield a fourfold increase in gain
    and a doubling of radar range.

18
3.4 Receiver sensitivity, Smin
  • Similar to that of transmitter power, increases
    in receiver sensitivity yield relatively small
    increases in radar range.
  • Only 19 range increase for a halving of
    sensitivity, and at the expense of false alarms.
  • Receiver design is a complex subject beyond the
    scope of this course, see 3.5.3.
  • Simplistically, the smaller the radar pulse
    width, the larger the required receiver bandwidth
    and the larger the receiver noise floor.

19
3.4.1 Receiver bandwidth
20
3.4.2 Signal-to-noise
21
3.4.3 Receiver threshold
22
4. Radar cross-section, ?
  • The radar cross-section of a target is a measure
    of its size as seen by a radar, expressed as an
    area, m2.
  • It is a complex function of the geometric
    cross-section of the target at the incident angle
    of the radar signal, as well as the directivity
    and reflectivity of the target.
  • The RCS is a characteristic of the target, not
    the radar.

23
4.1.1 RCS of a metal plate
  • Large RCS, but decreases rapidly as the incident
    angle deviates from the normal.

24
4.1.2 RCS of a metal sphere
  • Small RCS, but is independent of incident angle.

25
4.1.3 RCS of a metal cylinder
  • RCS can be quite small or fairly large depending
    on orientation.

26
4.1.4 RCS of a trihedral corner reflector
  • The RCS of a trihedral (corner) is both large and
    relatively independent of incident angle.

27
5. Low Observability
  • From the previous discussion on the radar
    cross-section of targets, it should be obvious
    that determining the radar cross-section of an
    airplane is a complicated task.
  • The art of designing an aircraft to specifically
    have a low RCS is known as low observability, or
    more commonly known as stealth.
  • Stealth is a relatively new technology,
  • even full RCS prediction is only 2 decades old.

28
5.1 History of stealth aircraft 1
29
5.2 Aircraft high RCS areas 1
30
5.3 Low observability design areas 1
31
5.3.1 Low observability design example1
32
5.3.2 Low observability design example1
33
5.4 Comparative RCS 1
34
6. In-class exercises
35
6.1 Quick response exercise 1
  • Think carefully about the derivation of the radar
    range equation just presented. Is there a
    potentially significant loss component missing?
  • Hint recall the simple link equation from your
    very early lectures.

36
6.2 Quick response exercise 2
  • Why have designers of stealth aircraft sought to
    blend the physical transitions / features of the
    aircraft?
  • Will reduction in your aircraft RCS alone make
    you invisible to the enemy?
  • How else might they find you?

37
6.3 Radar range equation calculation
38
6.3 Radar range equation calculation
  • The US Navy AN/SPS-48 Air Search Radar is a
    medium-range, three-dimensional (height, range,
    and bearing) air search radar.
  • Published technical specifications include
  • Operating frequency 2900-3100 MHz
  • Transmitter peak power 60-2200 kW
  • PRF 161-1366 Hz, and pulse widths of 9 / 3 µsec
  • Phased array antenna with a gain of 38.5 dB
  • For its published maximum range of 250 miles for
    a nominal target such as the F-18, what is the
    receiver chain sensitivity in bBm?

39
References
  • Moir Seabridge, Military Avionics Systems,
    American Institute of Aeronautics Astronautics,
    2006. Sections 2.6 2.7
  • David Adamy, EW101 - A First Course in Electronic
    Warfare, Artech House, 2000. Chapters 3,4 6
  • George W. Stimson, Introduction to Airborne
    Radar, Second Edition, SciTch Publishing, 1998.
  • Principles of Radar Systems, student laboratory
    manual, 38542-00, Lab-Volt (Quebec) Ltd, 2006.
  • John C. Vaquer, US Navy Surface Officer Warfare
    School Documents, Combat Systems Engineering
    Radar, http//www.fas.org/man/dod-101/navy/docs/sw
    os/cmd/fun12/12-1/sld001.htm
  • Mark A. Hicks, "Clip art licensed from the Clip
    Art Gallery on DiscoverySchool.com"
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