Geiger-Mueller
These are the most common "Geiger
Counter" sensors. They are biased with enough voltage so that
when an atomic particle gets into the gas it causes an avalanche.
The size of the output pulse is the same no matter what the energy of
the input particle. Although it's possible to turn down the
voltage so that the output pulse has a relation to the input particle
energy, the operation is then no longer called Geiger Mueller.
There is a plateau in the count rate vs. applied voltage plot for a G-M
tube and it should be operated on the plateau, not above or
below. The recomended voltage for most tubes is in the 500 to 900
volt area.
After the particle leaves the tube there is a recovery time. If
another particle enters the tube before the recovery time has passed
the tube will conduct continuously. This is bad because most
Geiger counters will show zero when in fact they should be showing full
scale.
The common G-M tube is a metallic cylinder with a wire insulated in the
center. One end typically has a mica window to allow alpha
particles to enter. But the end area is much smaller than the
active area of a pancake type G-M tube. Pancake G-M tubes are
much more sensitive to alpha as well as beta and gamma rays than the
cylindrical type tubes.
The end of a "hot dog" type G-M tube or the face of a "pancake" tube
typically has a thin mica window. Ideally for the detection of
alpha particles there would be no window, but then the gas in the tube
would except. The density of the window puts a limit on the
energy level of the alpha particles that can get into the tube
(typically around 3 Mev).
Google "
Geiger
Mueller"
The sensivity of a G-M type tube can be greatly increased by adding
more electrodes.
2397071 Radiation Detector, Gerhard Herzog (Texaco - oil wells) -
multiple cathode disks and multiple anode wires
2397072 Radiation Detector - multiple cathode disks and multiple anode
wires
2397073 Radiation Detector - 5 to 10 times more sensitive than G-M
tube, uses more electrodes, but has some volumes where the field is
zero, hence there's a better way
2397074 Radiation Detector - very rugged
2397075 Radiation Detector - minimizes anode to cathode leakage (noise)
2873399 Radiation Detector - has no zero field volumes so is somewhat
more sensitive than 5 to 10 times a G-M tube
Calls:
2599352 Radiation Detector - greater cathode area by adding fins - more
sensitive
2649554 Radiation Indicator, Anton - (beta & gamma dosemeter)
2699513 Radiation Detector -multiple anode wires in addition to
increased cathode area
Scintillator
Some crystal or plastic that generates
a photon of light when hit by a particle is coupled with a photo
multiplier tube and both enclosed in a light tight package. The
output pulse is proportional to the energy of the input particle.
Ionization Chamber
An insulating chamber with some gas the
ionizes under the influence of strong radiation. Many of the
surplus civil defense survey meters (often erroneously called geiger
counters) use this type of detector.
spinthariscope
This is a hand held magnifier focused
on a screen made of Silver activated Zinc Sulfide and with an alpha
emitter source like Po-210 Polonium (Anti-Static Brush) or AM-241
(Smoke Detector). With a night adapted eye you can see the
scintillation. These show up on eBay, new from United Nuclear,
old from antique instrument dealers.
Others
There are many other ways of detecting
atomic radiation.
Dose Meters
While Geiger counters measure the rate
(i.e. counts per minute) a dose meter adds up the counts giving a total
exposure. These are usually in the form of badges that may have
photographic film or electronic integrators or pen shaped electrometers.
X-Ray
One way to detect X-Rays is to use a
Scintillator coupled to a photomultiplier tube in a light tight
manner. This was the method used on first generation CAT
scanners. The problem is that you can only have a small number of
these around the circumference of a circle and so the spacial
resolution is low. GE developed X-Ray sensors using Xenon gas
that can have many more sensors in the same space where there were only
a few photomultiplier types. As of 2008 this is a hot bed of
activity since CAT is the prefered method of imaging many things in the
human body (i.e. is prefered over MRI which is good for other things).
4031396 X-ray Detector, GE - multiple anode wires in a curved chamber
for CAT scanner
4707607 High Resolution X-Ray Detector, GE - an even higher resolution
detector using a flow of Xenon gas through the curved chamber for CAT
scanner
7355181 Radiological imaging apparatus and radiological imaging method
and radiological imaging support method, Hitachi - combines CAT and PET
images
US 2007/0147576 A1 - X-Ray CT Apparatus
and an Image Controlling Method Thereof, Toshiba - An X-ray CT
apparatus and image controlling method thereof that
achieves a higher time resolution tomography image on a region of
interest (ROI) of an object while reducing a total amount of X-ray
irradiation exposure.
Geiger Counter ............................. 250 / 374+
Design ................................. D10 / 47
In nuclear reactions ................... 376 / 254
Geiger Muller Tube ......................... 313 / 93
Survey meter ........................... 250 / 374+
With circuit ........................... 250 / 374+
1181423
Apparatus for Measuring Rontgen Rays,
May 2, 1916, K Bangert,
250/385.1
; 313/523;
313/93
1589833
Measuring Device for Electromagnetic Waves, H Behnken, June 22, 1926,
313/538
; 250/374;
313/93; 378/207; 378/82; 378/98 - X-Ray
detector
1855669
Method and Apparatus for the Measurement of Radiation Intensity, April
26, 1932,
250/377 ; 313/93; 324/109; 324/702; 324/97
1961708
System for Influencing an Electric Current by Irradiation, F M Penning,
June 5, 1934,
250/214.1 ; 313/538; 313/93; 315/150; 315/157;
315/337
1961717
Ray Intensity Meter System, C H Thomas, June 5, 1934,
378/97 ;
250/214R; 250/382; 313/601; 313/93; 315/150; 315/157; 315/234;
315/241R; 361/175
1995018
Gas Filled Tube, H J Spanner, March 19, 1935
313/592 ; 313/253;
313/594; 313/93; 315/105; 315/268
2257827
Electron Discharge Tube, G J Weissenberg, October 7, 1941,
445/35
; 313/149; 313/355; 313/485; 313/93; 427/111; 427/74
2390965 Central Electrode Support, S A Scherbatskoy,
December 11,
1945, 250/374 ; 174/152E; 250/256; 313/246; 313/247;
313/255; 313/292; 313/318.01; 313/357; 313/545; 313/93
2521315
Geiger Tube, J A Victoreen, September 5, 1950,
313/93
; 313/278; 313/286; 313/290; 313/552 - improved quenching
2542440
Geiger Tube, J A Victoreen, February 20, 1951,
313/93 ;
220/2.3R; 313/247; 313/281 - Mica end window
Calls:
249064
Receiver for Telephones, R M Lockwood, November 1, 1881,
181/167
454941
Phonograph Recorder or Reproducer, T A Edison, June 30, 1891,
181/162
; 181/170
2159628
Telephone Transmitter, E G Danielson, May 23, 1939,
381/174 ;
181/167; 264/320; 425/DIG.56
2475603
Geiger Counter Structure, H Friedman, July 12, 1949,
313/93 ;
313/312; 313/622
4721857
Sampling and recording dose rate meter 250/374 ; 250/376; 250/377
4859853
Solid
Gamma Ray Dosimeter which measures
radiation in terms of absorption in a material different from the
detector
material
5665970
Directional
Radiation Detector and Imager
4853163
Method of controlling discharge of stored electric charge in plastic
objects and forming Lichtenberg figures in plastic objects
264/406
; 264/101; 264/162; 264/340; 264/341; 264/40.1; 264/78; 428/13
This is the 03608 hits since time
this
page has been accessed since since 19 Jan 2006.