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**DOPPLER SHIFT**

Doppler is the apparent change in wavelength (or frequency) of an electromagnetic or acoustic wave when there
is relative movement between the transmitter (or frequency source) and the receiver.

Summary RF Equation for the Two-Way (radar) case

Summary RF Equation for the One-Way (ESM) case

Rules of Thumb for two-way signal travel

(divide in half for one-way ESM signal measurements)

At 10 GHz, f_{D} ≈

35 Hz per Knot

19 Hz per km/Hr

67 Hz per
m/sec

61 Hz per yd/sec

20 Hz per ft/sec

To estimate f

_{D} at other frequencies, multiply these by:

The Doppler effect is shown in Figure 1. In everyday life this effect is commonly noticeable when a whistling
train or police siren passes you. Audio Doppler is depicted, however Doppler can also affect the frequency of a
radar carrier wave, the PRF of a pulse radar signal, or even light waves causing a shift of color to the observer.

How do we know the universe is expanding?

Answer: The color of light from distant stars is shifted
to red (see Section 7-1: higher 8 or lower frequency means Doppler shift is stretched, i.e. expanding).

A
memory aid might be that the lights from a car (going away) at night are red (tail lights)!

Doppler
frequency shift is directly proportional to velocity and a radar system can therefore be calibrated to measure
velocity instead of (or along with) range. This is done by measuring the shift in frequency of a wave caused by an
object in motion (Figure 2).

* Transmitter in motion

* Reflector in motion

* Receiver in motion

* All three

For a closing relative velocity:

* Wave is compressed

* Frequency is increased

For an opening relative velocity:

* Wave is stretched

* Frequency is decreased

To compute Doppler frequency we note that velocity is range rate; V = dr/dt

For
the reflector in motion case, You can see the wave compression effect in Figure 3 when the transmitted wave peaks
are one wavelength apart. When the first peak reaches the target, they are still one wavelength apart (point a).

When the 2nd peak reaches the target, the target has advanced according to its velocity (vt) (point b), and
the first reflected peak has traveled toward the radar by an amount that is less than the original wavelength by
the same amount (vt) (point c).

As the 2nd peak is reflected, the wavelength of the reflected wave is 2(vt)
less than the original wavelength (point d).

The distance the wave travels is twice the target range. The
reflected phase lags transmitted phase by 2x the round trip time.

For a fixed target the received phase
will differ from the transmitted phase by a constant phase shift. For a moving target the received phase will
differ by a changing phase shift.

For the closing target shown in Figure 3, the received phase is advancing
with respect to the transmitted phase and appears as a higher frequency.

Doppler
is dependent upon closing velocity, not actual radar or target velocity as shown in Figure 4.

For the
following equations (except radar mapping), we assume the radar and target are moving directly toward one another
in order to simplify calculations (if this is not the case, use the velocity component of one in the direction of
the other in the formulas).

For the case of a moving reflector, doppler
frequency is proportional to 2x the transmitted frequency:

Higher rf = higher doppler shift

f

_{D}
= (2 x V

_{Target})(f/c)

Likewise, it can be shown that for other cases, the following relationships hold:

For
an airplane radar with an airplane target (The "all three moving" case)

f

_{D} = 2(V

_{Radar}
+ V

_{Target})(f/c)

For the case of a semi-active missile receiving signals
(Also "all three moving")

f

_{D} = (V

_{Radar} + 2V

_{Target} +V

_{Missile})(f/c)

For the airplane radar with a ground target (radar mapping) or vice versa.

f

_{D} = 2(V

_{Radar} Cosθ Cosф)(f/c), Where 2 and N are the radar scan azimuth and depression
angles.

For a ground based radar with airborne target - same as previous using
target track crossing angle and ground radar elevation angle.

For the ES/ESM/RWR case
where only the target or receiver is moving (One-way doppler measurements)

f

_{D} = V

_{Receiver
or Target} (f/c)

Note: See Figure 4 if radar and target are not moving directly towards or away from
one another.

Figure
5 depicts the results of a plot of the above equation for a moving reflector such as might be measured with a
ground radar station illuminating a moving aircraft. It can be used for the aircraft-to-aircraft case, if the
total net closing rate of the two aircraft is used for the speed entry in the figure. It can also be used for the
ES/ESM case (one-way doppler measurements) if the speed of the aircraft is used and the results are divided by
two.

SAMPLE PROBLEMS:

(1) If a ground radar operating at 10 GHz is tracking an airplane flying at a speed of 500 km/hr tangential to
it (crossing pattern) at a distance of 10 km, what is the Doppler shift of the returning signal?

Answer:
Since the closing velocity is zero, the Doppler is also zero.

(2) If the same aircraft turns directly
toward the ground radar, what is the Doppler shift of the returning signal?

Answer: 500 km/hr = 270 kts from Section 2-1. From Figure 4 we see that the Doppler frequency is

about 9.2 KHz.

(3) Given that a ground radar operating at 7 GHz is Doppler tracking an aircraft 20 km away
(slant range) which is flying directly toward it at an altitude of 20,000 ft and a speed of 800 ft/sec, what
amount of VGPO switch would be required of the aircraft jammer to deceive (pull) the radar to a zero Doppler
return?

Answer: We use the second equation from the bottom of page 2-6.3 which is essentially the same for

this application except a ground based radar is tracking an airplane target (versus an

airplane during ground mapping), so for our application we use a positive elevation angle

instead of a negative (depression) angle.

f

_{D} = 2(V

_{r} Cos θ Cos ф)(f/c),
where θ is the aircraft track crossing angle and ф is the radar elevation angle.

Since the aircraft is
flying directly at the radar, 2 = θ°; the aircraft altitude = 20,000 ft = 6,096 meters.

Using the angle
equation in Section 2-1, sin ф = x/r = altitude / slant range, so:

ф = sin

^{-1} (altitude/slant
range) = sin

^{-1} (6,096 m / 20,000 m) = 17.7°

F

_{D} = 2(800 ft/sec Cos θ° Cos 17.7°)(7x10
Hz

^{9} / 9.8357 x 10

^{9} ft/sec) =

10,845 Hz
**Table of Contents
for Electronics Warfare and Radar Engineering Handbook**

Introduction |
Abbreviations | Decibel | Duty
Cycle | Doppler Shift | Radar Horizon / Line
of Sight | Propagation Time / Resolution | Modulation
| Transforms / Wavelets | Antenna Introduction
/ Basics | Polarization | Radiation Patterns |
Frequency / Phase Effects of Antennas |
Antenna Near Field | Radiation Hazards |
Power Density | One-Way Radar Equation / RF Propagation
| Two-Way Radar Equation (Monostatic) |
Alternate Two-Way Radar Equation |
Two-Way Radar Equation (Bistatic) |
Jamming to Signal (J/S) Ratio - Constant Power [Saturated] Jamming
| Support Jamming | Radar Cross Section (RCS) |
Emission Control (EMCON) | RF Atmospheric
Absorption / Ducting | Receiver Sensitivity / Noise |
Receiver Types and Characteristics |
General Radar Display Types |
IFF - Identification - Friend or Foe | Receiver
Tests | Signal Sorting Methods and Direction Finding |
Voltage Standing Wave Ratio (VSWR) / Reflection Coefficient / Return
Loss / Mismatch Loss | Microwave Coaxial Connectors |
Power Dividers/Combiner and Directional Couplers |
Attenuators / Filters / DC Blocks |
Terminations / Dummy Loads | Circulators
and Diplexers | Mixers and Frequency Discriminators |
Detectors | Microwave Measurements |
Microwave Waveguides and Coaxial Cable |
Electro-Optics | Laser Safety |
Mach Number and Airspeed vs. Altitude Mach Number |
EMP/ Aircraft Dimensions | Data Busses | RS-232 Interface
| RS-422 Balanced Voltage Interface | RS-485 Interface |
IEEE-488 Interface Bus (HP-IB/GP-IB) | MIL-STD-1553 &
1773 Data Bus |

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