Transcript Slide 1

A short history of Radar up to 1945
How some mathematical calculations, plus a lot of science
helped to win the war
Chris Budd, G4NBG
Where Radar Started
The best equation of all
Maxwell and the discovery of electromagnetic waves
E 
.D  ,
B
D
 M,   H  
 J,
t
t
.B  0.
Radar before Radar
Hertz: Practical demonstration of radio waves (50cm)
and that they were reflected from metallic objects
Marconi: Invention of radio communication (long wave)
In 1899 he proposed used of CW Radio to detect ships in fog and
demonstrated by Christian Huelsmeyer 1904 then used on the
Normandie
1930s Set up of commercial radio stations
Complaints by listeners of interference when aeroplanes flew near.
Report on reflected radio waves by Post Office Engineers 1933.
The British Invention of Radar
Problem: vulnerability of UK to bombing attack:
‘The bomber will always get through’ Baldwin
1934: Defence committee set up: Tizard. Rowe, Blackett, Wimperis
Q. 1935 : Could a bomber be destroyed by a radio ‘death ray’
Sir Robert Watson Watt (NPL), showed by
calculation that this was not possible, as it
required 5 GW of power
BUT calculations (by Wilkins) showed that
radio waves scattered by an aircraft could
be detected.
Worried about a factor of 10
This indicated that the aircraft and its range
could be found
12th Feb 1935
'Detection and location of aircraft
by radio methods’
Watson-Watt
The basic physics behind the early radar
Dipole aerial …. This is a transmitter and also a reflector of radio waves
current I_0
Radiation pattern


cos cos( )
i I0
2
 i(tkr)
E 
e
,
2 0 c r
sin( )


cos cos( )
60I0
2

E 
r
sin( )
The maths behind the memorandum: how maths won the war!
25m


cos cos( )
60I0
2

ET 
r
sin( )

6km
A. Wilkins
30 MHz
Field at target
ET 14m V m1 per amp of antenna current
Current in target wing I = 1.5 mA per amp of antenna current
Received field E r 15V m per amp of antenna current

1
Amp = 15A .. So received field E  255V m which is detectable!
1
A question of power
P: Transmitter power (100 kW) wavelength
Power reaching aircraft at range r:
GPA
4 r 2
Reflected power:
Power reaching receiver:

Power received:
GP
2
4

r


GPA

16 2 r 4
G 2 PA 2
Pr 
64 3 r 4
If r = 10km then received power is in pico Watts!

26th Feb 1935: Daventry Experiment
49.8m
Sir Hugh Dowding
Heyford
bomber
£10 000
1935-1939 Orfordness, Bawdsey and pulsed radar
E G Bowen .. Airborne radar 200MHz
Pulsed radar gives range = c t
Chain Home: Good Friday 1939
20 stations operational: 400kW
100 mile range … Gave 30 mins warning
13m Horizontal polarisation
350ft
Estimation of height

R

h


h 107R  0.88R2
h1

h2


elevation angle deg
h height in feet
R range in nMiles
Curvature of earth
correction
2 h1

sin
sin( )
 


2 h2

sin
sin( )
 

Operator measures strength of

two signals
at antennae at two
different heights to find

Chain Home and the Battle of Britain
July-Sept 1940. 15th Sept = Battle of Britain Day
K. Park and H. Dowding
600 RAF vs. 2000 Luftwaffe
Germans dismissed Radar thinking that a ground station could only
control one aircraft at a time!!
In contrast Radar was part of a major organisation
Aircraft detected using a mixture of statistics
and trigonometry
Position
combining the
two
Projected
position using
trigonometry
Last known
position of
German aircraft
Estimates of
position
from Radar
stations
Never in the
field of human
conflict was so
much owed by
so many to so
few.
Operations room 11 Group Uxbridge
Problems with the original Radar Systems
• 13m / 30 MHz wavelength gave poor resolution
• lots of ground clutter
• poor directional finding … RDF
• too large to fit easily in an aircraft
Solution .. Use much smaller wavelength eg. 10cm, 3GHz
But .. Problems with existing Klystron valves (TRE) generating
enough power at microwave frequencies
The Birmingham Connection: The Cavity Magnetron
Oliphant, Randall
and Boot:
21/02/1940
University of
Birmingham/GEC
Kilowatts of power at
centimetric wavelengths!
E B
v
B2

Tizard Mission
September 1940
British scientific secrets taken to America
15kW Magnetron no. 12 .. E G Bowen
(Jet Engine and Atomic Bomb)
Developed in the MIT
radiation lab: 10cm
airborne radar
(Lawrence)
Airborne Interception Radar (AI)
Early 1.5m/200MHz radar
AI mark IV
German Ai radar
Bowen!!
1 micro second pulse width .. 1
mile/speed of light
H2S Radar April 1942
TRE Malvern: A Rowe
Blumlein, Dee, Rowe, Lovell
German Radar
Freya
Wurzburg
Major use of
Bletchley
Intercepts!!
Bruneval
R V Jones
Other uses of Radar
Anti Submarine Radar
Radar based navigation: Oboe
Jamming: Window/Chaff
What RADAR led to
Radio Astronomy
Hey: Radio interference from the sun
Lovell: Jodrell Bank
Microwave cooking
Microwave communication and the mobile phone